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Research article Special Issues

Rich and complex dynamics of a time-switched differential equation model for wild mosquito population suppression with Ricker-type density-dependent survival probability

  • Received: 17 August 2023 Revised: 27 September 2023 Accepted: 29 September 2023 Published: 20 October 2023
  • MSC : 34A25, 34K13, 34K45, 92D25, 92D30, 92D40

  • Dengue presents over 390 million cases worldwide yearly. Releasing Wolbachia-infected male mosquitoes to suppress wild mosquitoes via cytoplasmic incompatibility has proven to be a promising method for combating the disease. As cytoplasmic incompatibility causes early developmental arrest of the embryo during the larval stage, we introduce the Ricker-type survival probability to assess the resulting effects. For periodic and impulsive release strategies, our model switches between two ordinary differential equations. Owing to a Poincaré map and rigorous dynamical analyses, we give thresholds T,c and c(>c) for the release period T and the release amount c. Then, we assume c>c and prove that our model admits a globally asymptotically stable periodic solution, provided T>T, and it admits at most two periodic solutions when T<T. Moreover, for the latter case, we assert that the origin is globally asymptotically stable if cc, and there exist two positive numbers such that whenever there is a periodic solution, it must initiate in an interval composed of the aforementioned two numbers, once c<c<c. We also offer numerical examples to support the results. Finally, a brief discussion is given to evoke deeper insights into the Ricker-type model and to present our next research directions.

    Citation: Zhongcai Zhu, Xue He. Rich and complex dynamics of a time-switched differential equation model for wild mosquito population suppression with Ricker-type density-dependent survival probability[J]. AIMS Mathematics, 2023, 8(12): 28670-28689. doi: 10.3934/math.20231467

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  • Dengue presents over 390 million cases worldwide yearly. Releasing Wolbachia-infected male mosquitoes to suppress wild mosquitoes via cytoplasmic incompatibility has proven to be a promising method for combating the disease. As cytoplasmic incompatibility causes early developmental arrest of the embryo during the larval stage, we introduce the Ricker-type survival probability to assess the resulting effects. For periodic and impulsive release strategies, our model switches between two ordinary differential equations. Owing to a Poincaré map and rigorous dynamical analyses, we give thresholds T,c and c(>c) for the release period T and the release amount c. Then, we assume c>c and prove that our model admits a globally asymptotically stable periodic solution, provided T>T, and it admits at most two periodic solutions when T<T. Moreover, for the latter case, we assert that the origin is globally asymptotically stable if cc, and there exist two positive numbers such that whenever there is a periodic solution, it must initiate in an interval composed of the aforementioned two numbers, once c<c<c. We also offer numerical examples to support the results. Finally, a brief discussion is given to evoke deeper insights into the Ricker-type model and to present our next research directions.



    Fractional differential equation theory comes with fractional calculus and is an abstract form of many engineering and physical problems. It has been widely used in system control, system identification, grey system theory, fractal and porous media dispersion, electrolytic chemistry, semiconductor physics, condensed matter physics, viscoelastic systems, biological mathematics, statistics, diffusion and transport theory, chaos and turbulence and non-newtonian fluid mechanics. Fractional differential equation theory has attracted the attention of the mathematics and natural science circles at home and abroad, and has made a series of research results. It has become one of the international hot research directions and has very important theoretical significance and application value.

    As an important research area of fractional differential equation, boundary value problems have attracted a great deal of attention in the last ten years, especially in terms of the existence of positive solutions, and have achieved a lot of results (see [1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20]). When the nonlinear term changes sign, the research on the existence of positive solutions progresses slowly, and relevant research results are not many (see [21,22,23,24,25,26,27,28,29,30,31,32,33]).

    In [21], using a fixed point theorem in a cone, Agarwal et al. obtained the existence of positive solutions for the Sturm-Liouville boundary value problem

    {(p(t)u(t))+λf(t,u(t))=0,t(0,1),α1u(0)β1p(0)u(0)=0,α2u(1)+β2p(0)u(1)=0,

    where λ>0 is a parameter, p(t)C((0,1),[0,)), αi,βi0 for i=1,2 and α1α2+α1β2+α2β1>0; fC((0,1)×[0,),R) and fM, for M>0,t[0,1],u0 (M is a constant).

    In [22], Weigao Ge and Jingli Ren studied the Sturm-Liouville boundary value problem

    {(p(t)u(t))+λa(t)f(t,u(t))=0,t(0,1),α1u(0)β1p(0)u(0)=0,α2u(1)+β2p(0)u(1)=0,

    where a(t)0 and λ>0 is a parameter. They removed the restriction fM, using Krasnosel'skii theorem, obtained some new existence theorems for the Sturm-Liouville boundary value problem.

    In [23], Weigao Ge and Chunyan Xue studied the same Sturm-Liouville boundary value problem again. Without the restriction that f is bounded below, by the excision principle and area addition principle of degree, they obtained three theorems and extended the Krasnosel'skii's compression-expansion theorem in cones.

    In [25], Yongqing Wang et al. considered the nonlinear fractional differential equation boundary value problem with changing sign nonlinearity

    {Dα0+u(t)+λf(t,u(t))=0,t(0,1),u(0)=u(0)=u(1)=0,

    where 2<α3, λ>0 is a parameter, Dα0+ is the standard Riemann-Liouville fractional derivative. f is allowed to change sign and may be singular at t=0,1 and r(t)fz(t)g(x) for some given nonnegative functions r,z,g. By using Guo-Krasnosel'skii fixed point theorem, the authors obtained the existence of positive solutions.

    In [28], J. Henderson and R. Luca studied the existence of positive solutions for a nonlinear Riemann-Liouville fractional differential equation with a sign-changing nonlinearity

    {Dα0+u(t)+λf(t,u(t))=0,t(0,1),u(0)=u(0)=u(n2)(0)=0,Dp0+u(t)|t=1=mi=1aiDq0+u(t)|t=ξi,

    where λ is a positive parameter, α(n1,n],nN,n3,ξiR for all i=1,...m,(mN),0<ξ1<ξ2<<ξm<1,p,qR,p[1,n2],q[0,p], Dα0+ is the standard Riemann-Liouville fractional derivative. With the restriction that f may be singular at t=0,1 and r(t)fz(t)g(t,x) for some given nonnegative functions r,z,g, applying Guo-Krasnosel'skii fixed point theorem, the existences of positive solutions are obtained.

    In [31], Liu and Zhang studied the existence of positive solutions to the boundary value problem for a high order fractional differential equation with delay and singularities including changing sign nonlinearity

    {Dα0+x(t)+f(t,x(tτ))=0, t(0,1){τ},x(t)=η(t), t[τ,0],x(0)=x(0)==x(n2)(0)=0, n3,x(n2)(1)=0,

    where n1<αn,n=[α]+1,Dα0+ is the standard Riemann-Liouville fractional derivative. The restriction on the nonlinearity f is as follows: there exists a nonnegative function ρC(0,1)L(0,1), ρ(t)0, such that f(t,x)ρ(t) and φ2(t)h2(x)f(t,v(t)x)+ρ(t)φ1(t)(g(x)+h1(x)), for  (t,x)(0,1)×R+, where φ1, φ2L(0,1) are positive, h1, h2C(R+0,R+) are nondecreasing, gC(R+0,R+) is nonincreasing, R+0=[0,+), and

    v(t)={1, t(0,τ],(tτ)α2n+1,t(τ,1).

    By Guo-krasnosel'skii fixed point theorem and Leray-Schauder's nonlinear alternative theorem, some existence results of positive solutions are obtained, respectively.

    In [33], Tudorache and Luca considered the nonlinear ordinary fractional differential equation with sequential derivatives

    {Dβ0+(q(t)Dγ0+u(t))=λf(t,u(t)),t(0,1),u(j)(0)=0,j=0,1,n2,Dγ0+u(0)=0,q(1)Dγ0+u(1)=10q(t)Dγ0+u(t)dη0(t),Dα00+u(1)=pi=110Dαi0+u(t)dηi(t),

    where β(1,2],γ(n1,n],nN,n3,pN,αiR,i=0,1p,0α1<α2<<αpα0<γ1,α01,λ>0,q:[0,1](0,) is a continuous function, fC((0,1)×[0,),R) may be singular at t=0 and/or t=1, and there exist the functions ξ,ϕC((0,1),[0,)), φC((0,1)×[0,),[0,)) such that ξ(t)f(t,x)ϕ(t)φ(t,x),t(0,1),x(0,) with 0<10ξ(s)ds<,0<10ϕ(s)ds<. By the Guo-Krasnosel'skii fixed point theorem, the existence of positive solutions are obtained.

    As can be seen from the above research results, fixed point theorems are still common tools to solve the existence of positive solutions to boundary value problems with sign changing nonlinearity, especially the Guo-Krasnosel'skii fixed point theorem. In addition, for boundary value problems of ordinary differential equations, Weigao Ge et al. removed the restriction that the nonlinear item bounded below. However, for fractional boundary value problems, from the existing literature, there are still many restrictions on nonlinear terms.

    Our purpose of this paper is to establish the existence of positive solutions of boundary value problems (BVPs for short) of the nonlinear fractional differential equation as follows

    {Dα0+u(t)+λf(t,u(t))=0,t(0,1),u(0)=u(0)=u(n2)(0)=u(n2)(1)=0,n3, (1.1)

    where n1<α<n, λ>0, f:[0,1]×[0,+)R is a known continuous nonlinear function and allowed to change sign, and Dα0+ is the standard Riemann-Liouville fractional derivative.

    In this paper, by the Guo-Krasnosel'skii fixed point theorem, the sufficient conditions for the existence of positive solutions for BVPs (1.1) are obtained under a more relaxed condition compared with the existing literature, as follows. Throughout this paper, we suppose that the following conditions are satisfied.

    H0: There exists a known function ωC(0,1)L(0,1) with ω(t)>0, t(0,1) and 10(1s)α2ω(s)ds<+, such that f(t,u)>ω(t), for t(0,1), uR.

    This paper is organized as follows. In Section 2, we introduce some definitions and lemmas to prove our major results. In Section 3, some sufficient conditions for the existence of at least one and two positive solutions for BVPs (1.1) are investigated. As applications, some examples are presented to illustrate our major results in Section 4.

    In this section, we give out some important definitions, basic lemmas and the fixed point theorem that will be used to prove the major results.

    Definition 2.1. (see[1]) Let φ(x)L1(a,b). The integrals

    (Iαa+φ)(x)def=1Γ(α)xa(xt)α1φ(t)dt,x>a,
    (Iαbφ)(x)def=1Γ(α)bx(tx)α1φ(t)dt,x<a,

    where α>0, are called the Riemann-Liouville fractional integrals of the order α. They are sometimes called left-sided and right-sided fractional integrals respectively.

    Definition 2.2. (see[1]) For functions f(x) given in the interval [a,b], each of the expressions

    (Dαa+f)(x)=1Γ(nα)(ddx)nxa(xt)nα1f(t)dt,n=[α]+1,
    (Dαbf)(x)=(1)nΓ(nα)(ddx)nbx(tx)nα1f(t)dt,n=[α]+1

    is called Riemann-Liouville derivative of order α, α>0, left-handed and right-handed respectively.

    Definition 2.3. (see [2]) Let E be a real Banach space. A nonempty, closed, and convex set PE is called a cone if the following two conditions are satisfied:

    (1) if xP and μ0, then μxP;

    (2) if xP and xP, then x=0.

    Every cone PE induces the ordering in E given by x1x2 if and only if x2x1P.

    Lemma 2.1. (see [3]) Let α>0, assume that u,Dα0+uC(0,1)L1(0,1), then,

    Iα0+Dα0+u(t)=u(t)+C1tα1+C2tα2++Cntαn

    holds for some CiR,i=1,2,,n, where n=[α]+1.

    Lemma 2.2. Let yC[0,1] and n1<α<n. Then, the following BVPs

    {Dα0+u(t)+y(t)=0,0<t<1,u(0)=u(0)=u(n2)(0)=u(n2)(1)=0,n3 (2.1)

    has a unique solution

    u(t)=10G(t,s)y(s)ds,

    where

    G(t,s)=1Γ(α){tα1(1s)αn+1(ts)α1,0st1,tα1(1s)αn+1,0ts1. (2.2)

    Proof. From Definitions 2.1 and 2.2, Lemma 2.1, we know

    u(t)=Iα0+y(t)+C1tα1+C2tα2++Cntαn=1Γ(α)t0(ts)α1y(s)ds+C1tα1+C2tα2++Cntαn,

    where CiR,i=1,2n.

    From u(0)=u(0)=u(n2)(0)=0, we get Ci=0,i=2,3n, such that

    u(n2)(t)=1Γ(αn+2)t0(ts)αn+1y(s)ds+C1Γ(α)Γ(αn+2)tαn+2,u(n2)(1)=1Γ(αn+2)10(1s)αn+1y(s)ds+C1Γ(α)Γ(αn+2).

    From u(n2)(1)=0, we get C1=1Γ(α)10(1s)αn+1y(s)ds, so that

    u(t)=1Γ(α)t0(ts)α1y(s)ds+tα1Γ(α)10(1s)αn+1y(s)ds=1Γ(α)t0[tα1(1s)αn+1(ts)α1]y(s)ds+1Γ(α)1ttα1(1s)αn+1y(s)ds=10G(t,s)y(s)ds.

    The proof is completed.

    Lemma 2.3. Let n1<α<n. The function G(t,s) defined by (2.2) is continuous on [0,1]×[0,1] and satisfies 0G(t,s)G(1,s) and G(t,s)tα1G(1,s) for t,s[0,1].

    Proof. From the definition (2.2), it's easy to know G(t,s) is continuous on [0,1]×[0,1]. Next, we prove that G(t,s) satisfies 0G(t,s)G(1,s).

    For 0st1,

    G(t,s)t=1Γ(α)(α1)(ts)α2[tα2(1s)αn+1tα2(1st)α21]1Γ(α)(α1)(ts)α2[(1s)3n1]0(n3).

    For 0ts1, obviously, G(t,s)t0. Such that, G(t,s) is an increasing function of t and satisfies 0G(t,s)G(1,s).

    At last, we prove that G(t,s) satisfies G(t,s)tα1G(1,s).

    For 0st1,

    G(t,s)tα1G(1,s)=1Γ(α)[tα1(1s)αn+1(ts)α1]tα1Γ(α)[(1s)αn+1(1s)α1]=1Γ(α)[(tts)α1(ts)α1]0.

    For 0ts1,

    G(t,s)G(1,s)=tα1(1s)αn+1(1s)αn+1(1s)α1tα1(1s)αn+1(1s)αn+1=tα1.

    The proof is completed.

    At the end of this section, we present the Guo-Krasnosel'skii fixed point theorem that will be used in the proof of our main results.

    Lemma 2.4. (see [34]) Let X be a Banach space, and let PX be a cone in X. Assume Ω1,Ω2 are open subsets of X with 0Ω1¯Ω1Ω2. Let F:PP be a comletely continuous operator such that either

    1) Fxx,xPΩ1,Fxx,xPΩ2; or

    2) Fxx,xPΩ1,Fxx,xPΩ2;

    holds. Then, F has a fixed point in P(¯Ω2Ω1).

    By a positive solution of BVPs (1.1), we mean a function u:[0,1][0,+) such that u(t) satisfies (1.1) and u(t)>0 for t(0,1).

    Let Banach space E=C[0,1] be endowed with x=max. Let I = [0, 1] , define the cone P\subset E by

    P = \{x\in E : x(t)\geq t^{\alpha-1} \Vert x \Vert, t \in I \}.

    Lemma 3.1. Let \lambda > 0 , \omega \in C(0, 1) \cap L(0, 1) with \omega(t) > 0 on (0, 1) , and n-1 < \alpha < n . Then, the following boundary value problem of fractional differential equation

    \begin{equation} \left \{ \begin{array}{l@{\quad}l} D_{{0^+}}^{\alpha}v(t)+\lambda \omega(t) = 0, 0 < t < 1, \\ v(0) = v'(0) \cdots = {v^{(n - 2)}}(0) = v^{(n - 2)}(1) = 0, n \geq 3 \end{array} \right. \end{equation} (3.1)

    has a unique solution

    \begin{equation} v(t) = \lambda\int_{0}^{1}G(t, s)\omega(s)ds \end{equation} (3.2)

    and

    \begin{equation} 0\leq v(t) \leq \lambda t^{\alpha-1} M, \end{equation} (3.3)

    where

    M = \frac{1}{\Gamma(\alpha)}\int_0^1 (1-s)^{\alpha -n+1} \omega(s) \, ds.

    Proof. From Lemma 2.2, let y(t) = \lambda \omega(t) , we have (3.2) immediately. In view of Lemma 2.3, we obtain

    \begin{eqnarray} 0 \leq v(t) & = & \lambda\int_{0}^{1}G(t, s) \omega(s)ds \\ & = & \lambda\frac{t^{\alpha -1}}{\Gamma(\alpha)} \int_0^1 (1-s)^{\alpha -n+1} \omega(s) \, ds -\lambda\frac{1}{\Gamma(\alpha)} \int_0^t (t-s)^{\alpha -1} \omega(s) \, ds \\ &\leq& \lambda\frac{t^{\alpha -1}}{\Gamma(\alpha)}\int_0^1 (1-s)^{\alpha -n+1} \omega(s) \, ds\\ & = &\lambda t^{\alpha -1}M. \end{eqnarray} (3.4)

    From (3.4), (3.3) holds.

    The proof is completed.

    Lemma 3.2. Suppose that v = v(t) is the solution of BVPs (3.1) and define the function g(t, u(t)) by

    \begin{equation} g(t, u(t)) = f(t, u(t))+ \omega(t). \end{equation} (3.5)

    Then, u(t) is the solution of BVPs (1.1), if and only if x(t) = u(t)+v(t) is the solution of the following BVPs

    \begin{equation} \left \{ \begin{array}{l@{\quad}l} D_{{0^+}}^{\alpha}x(t)+\lambda g(t, x(t)-v(t)) = 0 \\ x(0) = x'(0) \cdots = {x^{(n - 2)}}(0) = x^{(n - 2)}(1) = 0, \; n \geq 3. \end{array} \right. \end{equation} (3.6)

    And when x(t) > v(t) , u(t) is a positive solution of BVPs(1.1).

    Proof. In view of Lemma 2.2, if u(t) and v(t) are the solutions of BVPs (1.1) and BVPs (3.1), respectively, we have

    \begin{eqnarray*} \nonumber D_{{0^+}}^{\alpha}\big(u(t)+v(t)\big) & = & D_{{0^+}}^{\alpha}u(t)+D_{{0^+}}^{\alpha}v(t) \\ & = & -\lambda f(t, u(t))-\lambda \omega(t) \\ & = & -\lambda[f(t, u(t))+\omega(t)] \\ & = & -\lambda g(t, u(t)), \end{eqnarray*}

    such that

    D_{{0^+}}^{\alpha}\big(u(t)+v(t)\big) +\lambda g(t, u(t)) = 0.

    Let x(t) = u(t)+v(t) , we have u(t) = x(t)-v(t) and

    D_{{0^+}}^{\alpha}x(t) +\lambda g(t, x(t)-v(t)) = 0.

    It is easily to obtain x(0) = x'(0) = x'(1) = 0 from the boundary conditions of BVPs (1.1) and BVPs (3.1).

    Hence, x(t) is the solution of BVPs (3.6).

    On the other hand, if v(t) and x(t) are the solution of BVPs (3.1) and BVPs (3.6), respectively. Similarly, u(t) = x(t)-v(t) is the solution of BVPs (1.1). Obviously, when x(t) > v(t) , u(t) > 0 is a positive solution of BVPs (1.1).

    The proof is completed.

    Lemma 3.3. Let T:P\rightarrow E be the operator defined by

    \begin{equation} Tx(t): = \lambda\int_{0}^{1}G(t, s)g(s, x(s)-v(s))ds. \end{equation} (3.7)

    Then, T:P\rightarrow P is comletely continuous.

    Proof. In view of the definition of the function g(t, u(t)) , we know that g(t, x(t)-v(t)) > 0 is continuous from the continuity of x(t) and v(t) .

    By Lemma 2.3, we obtain

    \begin{eqnarray*} \nonumber \Vert Tx \Vert = \max\limits_{t\in[0, 1]}\vert\lambda\int_{0}^{1}G(t, s)g(s, x(s)-v(s))ds\vert = \lambda\int_{0}^{1}G(1, s)g(s, x(s)-v(s))ds. \end{eqnarray*}

    So that, for t \in [0, 1] ,

    \begin{eqnarray*} \nonumber Tx(t) = \lambda \int_{0}^{1}G(t, s)g(s, x(s)-v(s))ds \geq t^{\alpha-1}\lambda\int_{0}^{1}G(1, s)g(s, x(s)-v(s))ds = t^{\alpha-1}\Vert Tx \Vert . \end{eqnarray*}

    Thus, T(P)\subset P .

    As the continuity and nonnegativeness of G(t, s) and H {_0} implies T is a continuous operator.

    Let \Omega \subset P be bounded, there exists a positive constant r > 0 , such that \vert x\vert\leq r , for all x\in\Omega . Set M_{0} = \max\limits_{0\leq x \leq r, t\in I}\mid f(t, x(t)-v(t))\mid , then,

    \left| {g(t, x(t) - v(t))} \right| \le \left| {f(t, x(t) - v(t))} \right| + \left| {\omega (t)} \right| \le {M_0} + \omega (t).

    So, for x\in \Omega and t\in [0, 1] , we have

    \begin{eqnarray*} \nonumber \left| {Tx(t)} \right| & = & \left| {\lambda \int_0^1 G (t, s)g(s, x(s) - v(s))ds} \right|\\ &\le& \lambda \left( {{M_0}\int_0^1 G (1, s)ds{\rm{ + }}\int_0^1 G (1, s)\omega (s)ds} \right)\\ &\le& \lambda \left( {{M_0}\int_0^1 G (1, s)ds{\rm{ + }}\frac{1}{{\Gamma (\alpha )}}\int_0^1 {\omega (s)ds} } \right). \end{eqnarray*}

    Hence, T is uniformly bounded.

    On the other hand, since G(t, s)\in C([0, 1]\times [0, 1]) , for \varepsilon > 0 , exists \delta > 0 , for t_{1}, t_{2} \in [0, 1] with \mid t_{1}-t_{2}\mid \le \delta , implies \left| {G({t_1}, s) - G({t_2}, s)} \right| < \frac{\varepsilon }{{\lambda \left({{M_0} + \int_0^1 {\omega (s)ds} } \right)}} , for s\in [0, 1].

    Then, for all x\in \Omega :

    \begin{array}{l} \left| {Tx({t_1}) - Tx({t_2})} \right|\\ = \left| {\lambda \int_0^1 G ({t_1}, s)g(s, x(s) - v(s))ds - \lambda \int_0^1 G ({t_2}, s)g(s, x(s) - v(s))ds} \right|\\ = \left| {\lambda \int_0^1 ( G({t_1}, s) - G({t_2}, s))g(s, x(s) - v(s))ds} \right|\\ \le \lambda \int_0^1 {\left| {G({t_1}, s) - G({t_2}, s)} \right|\left| {g(s, x(s) - v(s))} \right|} ds\\ \le \lambda \int_0^1 {\left| {G({t_1}, s) - G({t_2}, s)} \right|} \left( {{M_0} + \omega (s)} \right)ds\\ < \lambda \int_0^1 {\frac{\varepsilon }{{\lambda \left( {{M_0} + \int_0^1 {\omega (s)ds} } \right)}}\left( {{M_0} + \omega (s)} \right)ds} \\ \le \lambda \frac{\varepsilon }{{\lambda \left( {{M_0} + \int_0^1 {\omega (s)ds} } \right)}}\int_0^1 {\left( {{M_0} + \omega (s)} \right)ds} = \varepsilon . \end{array}

    Hence, T (\Omega) is equicontinuous. By Arzelà-Ascoli theorem, we have T:P \rightarrow P is completely continuous.

    The proof is completed.

    A function x(t) is said to be a solution of BVPs (3.6) if x(t) satisfies BVPs (3.6). In addition, if x(t) > 0 , for t\in(0, 1) , x(t) is said to be a positive solution of BVPs (3.6). Obviously, if x(t)\in P , and x(t)\neq 0 is a solution of BVPs (3.6), by x(t)\geq t^{\alpha-1}\vert x \vert , then x(t) is a positive solution of BVPs (3.6). By Lemma 3.2, if x(t) > v(t) , u(t) = x(t)-v(t) is a positive solution of BVPs (1.1).

    Next, we give some sufficient conditions for the existence of positive solutions.

    Theorem 3.1. For a given 0 < \eta < 1 , let I_{\eta} = [\eta, 1] . If

    H _{1} : \lim\limits_{x\rightarrow +\infty} \inf\limits_{t\in I_{\eta}}\frac{f(t, x)}{x} = +\infty

    holds, there exists \lambda^{*} > 0 , for any 0 < \lambda < \lambda^{*} , the BVPs (1.1) has at least one positive solution.

    Proof. By Lemma 3.2, if BVPs (3.6) has a positive solution x(t) and x(t) > v(t) , BVPs (1.1) has a positive solution u(t) = x(t)-v(t) . We will apply Lemma 2.4 to prove the theorem.

    In view of the definition of g(t, u(t)) , we have g(t, u(t))\geq 0 , so that BVPs (3.6) has a positive solution, if and only if the operator T has a fixed point in P .

    Define

    g_{1}(r_{1}) = \sup \limits_{t\in I, 0\leq x \leq r_{1}} g(t, x),

    where r_{1} > 0 .

    By the definition of g_{1}(r_{1}) and H _{1} , we have

    \lim\limits_{r_{1}\rightarrow +\infty} \frac{r_{1}}{g_{1}(r_{1})} = 0.

    Then, there exists R_{1} > 0 , such that

    \frac{R_{1}}{g_{1}(R_{1})} = \max\limits_{r_{1} > 0}{\frac{r_{1}}{g_{1}(r_{1})}}.

    Let L = g_{1}(R_{1}) , \lambda^{*} = \min \{\frac{R_{1}}{M}, \frac{(\alpha-1)\Gamma(\alpha+1)R_{1}}{L}\} , where \int_{0}^{1}G(1, s)ds = \frac{1}{(\alpha-1)\Gamma(\alpha+1)} .

    In order to apply Lemma 2.4, we separate the proof into the following two steps.

    Step 1:

    For every 0 < \lambda < \lambda^{*} , t\in I let \Omega_{1} = \{x\in E:\Vert x \Vert < R_{1}\} . Suppose x\in P\cap\partial\Omega_{1} , we obtain

    \begin{eqnarray*} R_{1}&\geq& x(t)-v(t)\geq t^{\alpha-1}\Vert x \Vert-\lambda t^{\alpha-1}M \\ & > & t^{\alpha-1}R_{1}-\frac{R_{1}}{M}t^{\alpha-1}M \\ & > & 0. \end{eqnarray*}

    So that

    g(t, x(t)-v(t))\leq g_{1}(R_{1}) = L

    and

    \begin{eqnarray*} \nonumber Tx(t) & = & \lambda \int_{0}^{1}G(t, s)g(s, x(x)-v(s))ds \\ &\le& \lambda \int_0^1 {G(1, s)g(s, x(s) - v(s))ds} \\ &\le& \lambda^{*} \int_0^1 {G(1, s){g_1}({R_1})ds} = \lambda^{*} L \int_0^1 {G(1, s)ds} \\ & < & \frac{(\alpha-1)\Gamma(\alpha+1)R_{1}}{L} \frac{L}{(\alpha-1)\Gamma(\alpha+1)} \\ & = & {R_1}. \end{eqnarray*}

    Therefore,

    \Vert Tx \Vert < \Vert x \Vert, x \in P \cap \partial \Omega_{1}.

    Step 2:

    From H_{1} , we know that

    \lim\limits_{x \rightarrow +\infty}\inf \limits_{t \in I_{\eta}} \frac{g(t, x)}{x} = \lim\limits_{x \rightarrow +\infty}\inf \limits_{t \in I_{\eta}} \frac{f(t, x)+\omega(t)}{x} = +\infty.

    Then, there exists R_{2} > (1+\eta^{1-\alpha})R_{1} > R_{1} , such that for all t \in I_{\eta} , when x > \frac{R_{2}}{1+\eta^{1-\alpha}} ,

    g(t, x) > \delta x,

    where \delta > \frac{1+\eta^{1-\alpha}}{\lambda N} > 0 , N = \int_{\eta}^{1}G(1, s)ds .

    Let \Omega_{2} = \{x \in E: \Vert x \Vert < R_{2} \} , for all x \in P \cap \partial \Omega_{2} , t \in I_{\eta} we have

    \begin{eqnarray*} \nonumber x(t)-v(t) &\geq & t^{\alpha-1}R_{2}-\lambda t^{\alpha-1} M \\ & > & t^{\alpha-1}R_{2}-\lambda^{*} t^{\alpha-1} M \\ &\geq & t^{\alpha-1}R_{2}-t^{\alpha-1} R_{1} \\ &\geq& \eta^{\alpha-1}(R_{2}-R_{1}) \\ & = & \frac{R_{2}}{1+\eta^{1-\alpha}} > 0. \end{eqnarray*}

    So that

    g(t, x(t)-v(t)) > \delta (x(t)-v(t)) > \delta \frac{R_{2}}{1+\eta^{1-\alpha}}

    and

    \begin{eqnarray*} \nonumber \Vert Tx \Vert & = & \max \limits_{t \in I} \lambda \int_{0}^{1}G(t, s)g(s, x(s)-v(s))ds\\ & = & \lambda \int_{0}^{1}G(1, s)g(s, x(s)-v(s))ds \\ & > & \lambda \int_{\eta}^{1}G(1, s)g(s, x(s)-v(s))ds \\ & > & \lambda \delta \frac{R_{2}}{1+\eta^{1-\alpha}} \int_{\eta}^{1}G(1, s)ds \\ & = & \lambda \delta \frac{R_{2}}{1+\eta^{1-\alpha}} N \\ & > & \lambda \frac{1+\eta^{1-\alpha}}{\lambda N} \frac{R_{2}}{1+\eta^{1-\alpha}} N \\ & = & R_{2}. \end{eqnarray*}

    Thus, \Vert Tx \Vert > \Vert x \Vert , for x \in P\cap \partial \Omega_{2} .

    Therefore, by the Lemma 2.4, the BVPs (3.6) has at least one positive solution x \in P \cap (\overline{\Omega_{2}}\setminus \Omega_{1}) , and R_{1} \leq \Vert x \Vert \leq R_{2} . From x(t)-v(t) > 0 , we know that BVPs (1.1) has at least one positive solution u(t) = x(t)-v(t) .

    The proof is completed.

    Theorem 3.2. Suppose

    H _{2} : \lim\limits_{x \rightarrow +\infty} \inf\limits_{t \in I_{\eta}} f(t, x) = +\infty;

    H _{3} : \lim\limits_{x \rightarrow +\infty} \sup\limits_{t \in I} \frac{f(t, x)}{x} = 0;

    hold, there exists \lambda^{*} > 0 , for all \lambda > \lambda^{*} , the BVPs (1.1) has at least one positive solution.

    Proof. Let \sigma = 2\frac{M}{N} . From H_{2} , we have

    \lim \limits_{x \rightarrow +\infty} \inf \limits_{t \in I_{\eta}} g(t, x) = \lim \limits_{x \rightarrow +\infty} \inf \limits_{t \in I_{\eta}} (f(t, x)+\omega(t)) = +\infty,

    such that for the above \sigma , there exists X > 0 , when x > X , for all t \in I_{\eta} , we obtain

    g(t, x) > \sigma.

    Let \lambda^{*} = \max\{\frac{N}{\eta^{\alpha-1}M}, \frac{X}{M}\} , R_{1} = 2\lambda M \eta^{1-\alpha} , where \lambda > \lambda^{*} . Let \Omega_{1} = \{x \in E: \Vert x \Vert < R_{1} \} , if x \in P \cap \partial \Omega_{1} , t \in I_{\eta} , we have

    \begin{eqnarray*} \nonumber x(t)-v(t) &\geq& t^{\alpha-1}R_{1}- \lambda t^{\alpha-1} M \\ & = & \eta^{\alpha-1}R_{1}- \lambda M \\ & = & \eta^{\alpha-1}\cdot 2 \lambda M \eta^{1-\alpha} - \lambda M = \lambda M \\ & > & \lambda^{*} M \geq X, \end{eqnarray*}

    such that

    g(t, x(t)-v(t)) > \sigma

    and

    \begin{eqnarray*} \nonumber \Vert Tx \Vert & = & \max\limits_{t \in I} \lambda \int_{0}^{1}G(t, s)g(s, x(s)-v(s))ds \\ & = & \lambda \int_{0}^{1}G(1, s)g(s, x(s)-v(s))ds \\ & > & \lambda \int_{\eta}^{1}G(1, s)g(s, x(s)-v(s))ds \\ & = & \lambda N \sigma = 2 \lambda \frac{M}{N} N = 2 \lambda M > R_{1}\\ & = & \Vert x \Vert. \end{eqnarray*}

    Hence, \Vert Tx \Vert > \Vert x \Vert , x \in P \cap \partial \Omega_{1} .

    On the other hand, from H_{3} , we know that there exists \varepsilon_{0} = \frac{{(\alpha - 1)\Gamma (\alpha + 1)}}{{2\lambda }} > 0 , R_{0} > R_{1} , for t\in[0, 1] , x > R_{0} , f(t, x) < {\varepsilon _0}x holds.

    Because of f \in C([0, 1] \times [0, + \infty), \mathbb{R}) , let \overline M = \mathop {\max }\limits_{(t, x) \in I \times [0, {R_0}]} \left\{ {f(t, x)} \right\} , then, for t \in[0, 1] , x\in[0, +\infty) , f(t, x) \le \overline M + {\varepsilon _0}x holds.

    Let {R_2} > \max \left\{ {{R_0}, \lambda M, \frac{{2\lambda \left({\overline M + \int_0^1 {\omega (s)ds} } \right)}}{{\Gamma (\alpha)}}} \right\} , {\Omega _2} = \{ x \in E:\left\| x \right\| < {R_2}\} , for x \in P \cap \partial {\Omega _2} and t\in[0, 1] , we have

    x(t) - v(t) \ge {t^{\alpha - 1}}{R_2} - \lambda {t^{\alpha - 1}}M{\rm{ = }}{t^{\alpha - 1}}({R_2} - \lambda M) \ge 0.

    So that,

    \begin{array}{l} g(t, x(t) - v(t)){\rm{ = }}f(t, x(t) - v(t)) + \omega (t)\\ \le \overline M + {\varepsilon _0}\left( {x(t) - v(t)} \right) + \omega (t)\\ \le \overline M + {\varepsilon _0}x(t) + \omega (t). \end{array}

    Therefore,

    \begin{array}{l} \left\| {Tx} \right\| = \mathop {\max }\limits_{t \in I} \lambda \int_0^1 G (t, s)g(s, x(s) - v(s))ds = \lambda \int_0^1 G (1, s)g(s, x(s) - v(s))ds\\ \le \lambda \int_0^1 G (1, s)\left( {\overline M + {\varepsilon _0}x(s) + \omega (s)} \right)ds\\ \le \lambda {\varepsilon _0}{R_2}\int_0^1 G (1, s)ds + \lambda \int_0^1 G (1, s)\left( {\overline M + \omega (s)} \right)ds\\ \le \lambda {\varepsilon _0}{R_2}\frac{1}{{(\alpha - 1)\Gamma (\alpha + 1)}} + \frac{\lambda }{{\Gamma (\alpha )}}\left( {\overline M + \int_0^1 {\omega (s)ds} } \right)\\ < \frac{{\lambda {R_2}}}{{(\alpha - 1)\Gamma (\alpha + 1)}}\frac{{(\alpha - 1)\Gamma (\alpha + 1)}}{{2\lambda }} + \frac{{{R_2}}}{2}\\ = {R_2}\\ = \left\| x \right\|. \end{array}

    So, we get

    \Vert Tx \Vert < \Vert x \Vert, x\in P \cap \partial \Omega_{2}.

    Hence, from Lemma 2.4, we know that the operator T has at least one fixed point x , which satisfies x \in P \cap (\overline{\Omega_{2}}\setminus \Omega_{1}) and R_{1} \leq \Vert x \Vert \leq R_{2} . From x(t)-v(t) > 0 , we know that BVPs (1.1) has at least one positive solution u(t) = x(t)-v(t) .

    The proof is completed.

    In this section, we provide two examples to demonstrate the applications of the theoretical results in the previous sections.

    Example 4.1. Consider the following BVPs

    \begin{equation} \left \{ \begin{array}{l@{\quad}l} D_{{0^+}}^{\frac{5}{2}}u + \lambda (u^{2}-e^{\sin t}-3t-2e) = 0, \\ u(0) = u'(0) = u'(1) = 0. \end{array} \right. \end{equation} (4.1)

    where \alpha = \frac{5}{2} , f(t, u) = u^{2}-e^{\sin t}-2e , \omega(t) = \frac{e^{\sin 10^{-1}}}{\sqrt{10}}t^{\frac{-1}{2}}+12e .

    Let \eta = 10^{-1} , then,

    g(t, u) = u^{2}-e^{\sin t}+\frac{e^{\sin 10^{-1}}}{\sqrt{10}}t^{\frac{-1}{2}}+10e,
    g_{1}(r) = \sup\limits_{t \in I_{\eta}, 0\leq u \leq r}g(t, u) = r^{2}+10e,

    and

    \lim\limits_{r \rightarrow +\infty} \frac{r}{g_{1}(r)} = \lim\limits_{r \rightarrow +\infty} \frac{r}{r^{2}+10e} = 0,

    R_{1} = \sqrt{10e} , L = g_{1}(R_{1}) = 20e , M = 16.7716 , N = 0.26667 , \frac{R_{1}}{M} = 0.310866 , \frac{(\alpha-1)\Gamma(\alpha+1)R_{1}}{L} = 0.478069 , \lambda^{*} = 0.310866 , R_{2} = 170.086 , N = 0.196967 .

    We can check that the condition of Theorem 3.1 is satisfied. Therefore, there exists at least one positive solution.

    Example 4.2. Consider the following BVPs

    \begin{equation} \left \{ \begin{array}{l@{\quad}l} D_{{0^+}}^{\frac{7}{3}}u + \lambda (e^{-t}u^{\frac{2}{3} }-t-10) = 0, \\ u(0) = u'(0) = u'(1) = 0. \end{array} \right . \end{equation} (4.2)

    where \alpha = \frac{7}{3} , f(t, u) = e^{-t}u^{\frac{2}{3} }-t-10 , \omega(t) = t^{\frac{-2}{3}}+10 .

    Let \eta = 0.3 , such that

    g(t, u) = e^{-t}u^{\frac{2}{3} }+t^{\frac{-2}{3}}-t,

    and M = 8.52480 , N = 0.219913 , \sigma = \frac{2M}{N} = 77.5290 , \frac{N}{\eta^{\alpha-1}M} = 0.128451 , R_{1} = 2\lambda M \eta^{-\frac{4}{3}} = 84.8957\lambda > 10.9049 .

    We can check that the conditions of Theorem 3.2 are satisfied. Therefore, there exists at least one positive solution.

    In this paper, the constraint on the nonlinear term is weakened to f(t, u) > -\omega(t) (where \omega(t) > 0 ). Under similar conditions, by constructing an auxiliary boundary value problem and using the principle of linear superposition, the difficulty caused by sign-change of nonlinear terms is overcome. Under the condition of singularity of nonlinear terms, the existence conclusions of positive solutions are obtained based on the Guo-Krasnosel'skii fixed point theorem.

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

    This research was supported by National Natural Science Foundation of China (Grant No. 12371308). The authors would like to thank the anonymous reviewers and the editor for their constructive suggestions on improving the presentation of the paper.

    The authors declares that they have no competing interest.



    [1] Dengue, World Mosquito Program, 2023. Available from: https://www.worldmosquitoprogram.org/en/learn/mosquito-borne-diseases/dengue.
    [2] A. Abidemi, J. Ackora-Prah, H. O. Fatoyinbo, J. K. K. Asamoah, Lyapunov stability analysis and optimization measures for a dengue disease transmission model, Phys. A, 602 (2022), 127646. https://dx.doi.org/10.1016/j.physa.2022.127646 doi: 10.1016/j.physa.2022.127646
    [3] A. Abidemi, H. O. Fatoyinbo, J. K. K. Asamoah, Analysis of dengue fever transmission dynamics with multiple controls: a mathematical approach, 2020 International Conference on Decision Aid Sciences and Application (DASA), 2020,971–978. https://dx.doi.org/10.1109/DASA51403.2020.9317064
    [4] L. Bai, L. C. Morton, Q. Liu, Climate change and mosquito-borne diseases in China: a review, Global. Health, 9 (2013), 10. https://dx.doi.org/10.1186/1744-8603-9-10 doi: 10.1186/1744-8603-9-10
    [5] L. Zou, J. Chen, X. Feng, S. Ruan, Analysis of a dengue model with vertical transmission and application to the 2014 dengue outbreak in Guangdong province, China, Bull. Math. Biol., 80 (2018), 2633–2651. https://dx.doi.org/10.1007/s11538-018-0480-9 doi: 10.1007/s11538-018-0480-9
    [6] W. Wang, B. Yu, X. Lin, D. Kong, J. Wang, J. Tian, et al., Reemergence and autochthonous transmission of dengue virus, eastern China, 2014, Emerg. Infec. Dis., 21 (2015), 1670–1673. https://dx.doi.org/10.3201/eid2109.150622 doi: 10.3201/eid2109.150622
    [7] Dengue and severe dengue, World Health Organization, 2023. Available from: https://www.who.int/health-topics/dengue-and-severe-dengue#tab = tab_1.
    [8] H. F. van Emden, M. W. Service, Pest and vector management, Cambridge University Press, 2004. https://dx.doi.org/10.1017/CBO9780511616334
    [9] J. K. K. Asamoah, E. Yankson, E. Okyere, G. Sun, Z. Jin, R. Jan, et al., Optimal control and cost-effectiveness analysis for dengue fever model with asymptomatic and partial immune individuals, Results Phys., 31 (2021), 104919. https://dx.doi.org/10.1016/j.rinp.2021.104919 doi: 10.1016/j.rinp.2021.104919
    [10] N. Becker, D. Petrić, M. Zgomba, C. Boase, M. Madon, C. Dahl, et al., Mosquitoes and their control, Spring-Verlag Berlin Heidelberg, 2010. https://dx.doi.org/10.1007/978-3-540-92874-4
    [11] J. Li, B. Song, X. Wang, An extended discrete Ricker population model with Allee effects, J. Differ. Equ. Appl., 13 (2007), 309–321. https://dx.doi.org/10.1080/10236190601079191 doi: 10.1080/10236190601079191
    [12] T. C. Iles, A review of stock-recruitment relationships with reference to flatfish populations, Neth. J. Sea Res., 32 (1994), 399–420. https://dx.doi.org/10.1016/0077-7579(94)90017-5 doi: 10.1016/0077-7579(94)90017-5
    [13] M. Hartmann, G. Hosack, R. Hillary, J. Vanhatalo, Gaussian process framework for temporal dependence and discrepancy functions in Ricker-type population growth models, Ann. Appl. Stat., 11 (2017), 1375–1402. https://dx.doi.org/10.1214/17-AOAS1029 doi: 10.1214/17-AOAS1029
    [14] G. Marinoschi, A. Martiradonna, Fish populations dynamics with nonlinear stock-recruitment renewal conditions, Appl. Math. Comput., 277 (2016), 101–110. https://dx.doi.org/10.1016/j.amc.2015.12.041 doi: 10.1016/j.amc.2015.12.041
    [15] W. H. So, J. S. Yu, Global attractivity and uniform persistence in Nicholson's blowflies, Differ. Equ. Dyn. Syst., 2 (1994), 11–18.
    [16] M. R. S. Kulenović, G. Ladas, Y. G. Sficas, Global attractivity in Nicholson's blowflies, Appl. Anal., 43 (1992), 109–124. https://dx.doi.org/10.1080/00036819208840055 doi: 10.1080/00036819208840055
    [17] K. Mark, Elements of mathematical ecology, Cambridge University Press, 2001. https://dx.doi.org/10.1017/CBO9780511608520
    [18] J. M. Murray, Mathematical biology, Springer-Verlag Berlin Heidelberg, 1989. https://dx.doi.org/10.1007/b98868
    [19] M. Sicard, M. Bonneau, M. Weill, Wolbachia prevalence, diversity, and ability to induce cytoplasmic incompatibility in mosquitoes, Curr. Opin. Insect Sci., 34 (2019), 12–20. https://dx.doi.org/10.1016/j.cois.2019.02.005 doi: 10.1016/j.cois.2019.02.005
    [20] R. Moretti, M. Calvitti, Issues with combining incompatible and sterile insect techniques, Nature, 590 (2021), E1–E2. https://dx.doi.org/10.1038/s41586-020-03164-w doi: 10.1038/s41586-020-03164-w
    [21] X. Zheng, D. Zhang, Y. Li, C. Yang, Y. Wu, X. Liang, et al., Incompatible and sterile insect techniques combined eliminate mosquitoes, Nature, 572 (2019), 56–61. https://dx.doi.org/10.1038/s41586-019-1407-9 doi: 10.1038/s41586-019-1407-9
    [22] T. Walker, P. Johnson, L. Moreira, I. Iturbe-Ormaetxe, F. D. Frentiu, C. J. McMeniman, et al., The wMel Wolbachia strain blocks dengue and invades caged Aedes aegypti populations, Nature, 476 (2011), 450–453. https://dx.doi.org/10.1038/nature10355 doi: 10.1038/nature10355
    [23] S. L. Dobson, W. Rattanadechakul, E. J. Marsland, Fitness advantage and cytoplasmic incompatibility in Wolbachia single- and superinfected Aedes albopictus, Heredity, 93 (2004), 135–142. https://dx.doi.org/10.1038/sj.hdy.6800458 doi: 10.1038/sj.hdy.6800458
    [24] D. Zhang, X. Zheng, Z. Xi, K. Bourtzis, J. R. L. Gilles, Combining the sterile insect technique with the incompatible insect technique: Ⅰ-impact of Wolbachia infection on the fitness of triple- and double-infected strains of Aedes albopictus, PloS One, 10 (2015), e0121126. https://dx.doi.org/10.1371/journal.pone.0121126 doi: 10.1371/journal.pone.0121126
    [25] D. Zhang, R. S. Lees, Z. Xi, K. Bourtzis, J. R. L. Gilles, Combining the sterile insect technique with the incompatible insect technique: Ⅲ-robust mating competitiveness of irradiated triple Wolbachia-infected Aedes albopictus males under semi-field conditions, PLoS One, 11 (2016), e0151864. https://dx.doi.org/10.1371/journal.pone.0151864 doi: 10.1371/journal.pone.0151864
    [26] J. Yu, Modelling mosquito population suppression based on delay differential equations, SIAM J. Appl. Math., 78 (2018), 3168–3187. https://dx.doi.org/10.1137/18M1204917 doi: 10.1137/18M1204917
    [27] J. Yu, J. Li, Global asymptotic stability in an interactive wild and sterile mosquito model, J. Differ. Equ., 269 (2020), 6193–6215. https://dx.doi.org/10.1016/j.jde.2020.04.036 doi: 10.1016/j.jde.2020.04.036
    [28] Z. Zhu, B. Zheng, Y. Shi, R. Yan, J. Yu, Stability and periodicity in a mosquito population suppression model composed of two sub-models, Nonlinear Dyn., 107 (2021), 1383–1395. https://dx.doi.org/10.1007/s11071-021-07063-1 doi: 10.1007/s11071-021-07063-1
    [29] Z. Zhu, X. Feng, L. Hu, Global dynamics of a mosquito population suppression model under a periodic release strategy, J. Appl. Anal. Comput., 13 (2023), 2297–2314. https://dx.doi.org/10.11948/20220501 doi: 10.11948/20220501
    [30] J. Hale, Ordinary differential equations, New York: John Wiley, 1980.
    [31] M. Han, X. Hou, L. Sheng, C. Wang, Theory of rotated equations and applications to a population model, Discrete Contin. Dyn. Syst., 38 (2018), 2171–2185. https://dx.doi.org/10.3934/dcds.2018089 doi: 10.3934/dcds.2018089
    [32] Dengue-Pakistan, World Health Organization, 2022. Available from: https://www.who.int/emergencies/disease-outbreak-news/item/2022-DON414.
    [33] Dengue-Nepal, World Health Organization, 2022. Available from: https://www.who.int/emergencies/disease-outbreak-news/item/2022-DON412.
    [34] S. B. Halstead, Dengue, Lancet, 370 (2007), 1644–1652. https://dx.doi.org/10.1016/S0140-6736(07)61687-0 doi: 10.1016/S0140-6736(07)61687-0
    [35] M. Tolle, Mosquito-borne diseases, Curr. Prob. Pediatr. Ad., 39 (2009), 97–140. https://dx.doi.org/10.1016/j.cppeds.2009.01.001 doi: 10.1016/j.cppeds.2009.01.001
    [36] N. W. Beebe, D. Pagendam, B. J. Trewin, S. A. Ritchie, Releasing incompatible males drives strong suppression across populations of wild and Wolbachia-carrying Aedes aegypti in Australia, Proc. Nati. Acad. Sci. USA, 118 (2021), e2106828118. https://dx.doi.org/10.1073/pnas.2106828118 doi: 10.1073/pnas.2106828118
    [37] J. Li, L. Cai, Y. Li, Stage-structured wild and sterile mosquito population models and their dynamics, J. Biol. Dyn., 11 (2016), 79–101. https://dx.doi.org/10.1080/17513758.2016.1159740 doi: 10.1080/17513758.2016.1159740
    [38] L. Cai, S. Ai, J. Li, Dynamics of mosquitoes populations with different strategies for releasing sterile mosquitoes, SIAM J. Appl. Math., 74 (2014), 1786–1809. https://dx.doi.org/10.1137/13094102X doi: 10.1137/13094102X
    [39] B. Zheng, J. Yu, At most two periodic solutions for a switching mosquito population suppression model, J. Dynam. Differ. Equ., 2022. https://dx.doi.org/10.1007/s10884-021-10125-y doi: 10.1007/s10884-021-10125-y
    [40] M. Huang, S. Liu, X. Song, Study of a delayed mosquito population suppression model with stage and sex structure, J. Appl. Math. Comput., 69 (2022), 89–111. https://dx.doi.org/10.1007/s12190-022-01735-w doi: 10.1007/s12190-022-01735-w
    [41] L. Hu, C. Yang, Y. Hui, J. Yu, Mosquito control based on pesticides and endosymbiotic bacterium Wolbachia, Bull. Math. Biol., 83 (2021), 58. https://dx.doi.org/10.1007/s11538-021-00881-9 doi: 10.1007/s11538-021-00881-9
    [42] Z. Zhang, B. Zheng, Dynamics of a mosquito population suppression model with a saturated Wolbachia release rate, Appl. Math. Lett., 129 (2022), 107933. https://dx.doi.org/10.1016/j.aml.2022.107933 doi: 10.1016/j.aml.2022.107933
    [43] Y. Chen, Y. Wang, J. Yu, B. Zheng, Z. Zhu, Global dynamics of a mosquito population suppression model with seasonal switching, Adv. Differ. Equ., 28 (2023), 889–920. https://dx.doi.org/10.57262/ade028-1112-889 doi: 10.57262/ade028-1112-889
    [44] J. Li, New revised simple models for interactive wild and sterile mosquito populations and their dynamics, J. Biol. Dyn., 11 (2017), 316–333. https://dx.doi.org/10.1080/17513758.2016.1216613 doi: 10.1080/17513758.2016.1216613
    [45] G. Lin, Y. Hui, Stability analysis in a mosquito population suppression model, J. Biol. Dyn., 14 (2020), 578–589. https://dx.doi.org/10.1080/17513758.2020.1792565 doi: 10.1080/17513758.2020.1792565
    [46] J. Adams, M. Jones, Estimation of lake-scale stock-recruitment models for Great Lakes sea lampreys, Ecol. Model., 467 (2022), 109916. https://dx.doi.org/10.1016/j.ecolmodel.2022.109916 doi: 10.1016/j.ecolmodel.2022.109916
    [47] Z. Liu, T. Chen, T. Zhou, Analysis of impulse release of Wolbachia to control Nilaparvata lugens, Commun. Nonlinear Sci. Numer. Simul., 116 (2023), 106842. https://dx.doi.org/10.1016/j.cnsns.2022.106842 doi: 10.1016/j.cnsns.2022.106842
    [48] L. Erdős, Green heroes: from Buddha to Leonardo DiCaprio, Cham: Springer, 2019. https://dx.doi.org/10.1007/978-3-030-31806-2
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