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Research article Special Issues

Transmission dynamics and optimal control of a Huanglongbing model with time delay


  • In this paper, a mathematical model has been formulated for the transmission dynamics of citrus Huanglongbing considering latent period as the time delay factor. Existence of the equilibria and their stability have been studied on the basis of basic reproduction number in two cases τ=0 and τ>0. The results show that stability changes occur through Hopf bifurcation in the delayed system. Optimal control theory is then applied to investigate the optimal strategy for curtailing the spread of the disease using three time-dependent control variables determined from sensitivity analysis. By using Pontryagin's Maximum Principle, we obtain the optimal integrated strategy and prove the uniqueness of optimal control solution. Analytical and numerical findings suggest that it is feasible to implement control techniques while minimizing the cost of implementation of optimal control strategies.

    Citation: Zhenzhen Liao, Shujing Gao, Shuixian Yan, Genjiao Zhou. Transmission dynamics and optimal control of a Huanglongbing model with time delay[J]. Mathematical Biosciences and Engineering, 2021, 18(4): 4162-4192. doi: 10.3934/mbe.2021209

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  • In this paper, a mathematical model has been formulated for the transmission dynamics of citrus Huanglongbing considering latent period as the time delay factor. Existence of the equilibria and their stability have been studied on the basis of basic reproduction number in two cases τ=0 and τ>0. The results show that stability changes occur through Hopf bifurcation in the delayed system. Optimal control theory is then applied to investigate the optimal strategy for curtailing the spread of the disease using three time-dependent control variables determined from sensitivity analysis. By using Pontryagin's Maximum Principle, we obtain the optimal integrated strategy and prove the uniqueness of optimal control solution. Analytical and numerical findings suggest that it is feasible to implement control techniques while minimizing the cost of implementation of optimal control strategies.



    Citrus Huanglongbing (HLB), currently the most economically destructive disease of citrus worldwide, is caused by phloem-restricted bacteria of the Candidatus Liberibacter group with symptoms including stunted growth and poor flowering of citrus trees as well as blotchy mottling and yellowing of their leaves [1,2,3]. It was first reported from southern China in 1919, with a history of more than a century in China [1]. Now it is distributed in nearly 50 countries and regions in Asia, Africa, North and South America, Europe, etc., and its occurrence scope is still expanding at present, which makes it true that over 80% of the planted area can not escape from being infected [4,5,6]. The infected trees are usually destroyed or become unproductive in 2 to 5 years [1,7]. To date, there is no good source of genetic resistance to HLB in the genus citrus, and the disease can not be cured once the trees are infected [8]. Therefore, HLB still pose a significant threat to the development of the citrus industry.

    Experimental studies have shown that early stages of HLB, the bacteria can remain undetectable in the trees after initial infection. It might take a 2 to 6 months latent period for the tree to become infectious before new psyllid generations can become infected [9]. HLB latency is highly variable and apparently greatly affected by tree age, horticultural health, and other factors. In order to be more precise description of HLB transmission in a citrus orchard, it is reasonable to incorporate time latency into the delayed system. Delay differential equations (DDEs) are one of the most powerful mathematical tools for studying the effect of delay in the dynamics of the disease [10,11,12,13,14,15]. For instance, AI Basir et al. [12] derived a mathematical model for the transmission dynamics of vector-borne plant disease considering incubation period as the time delay factor. Fan et al. [14] formulated a delay differential equation model for the transmission of West Nile virus between vector mosquitoes and avian hosts that incorporates maturation delay for mosquitoes. They found that a combination of the maturation delay and the vertical transmission of the virus in mosquitoes has substantial influence on the abundance and number of infection peaks of the infectious mosquitoes. Vilamiu et al. [15] presented a delayed HLB model and assess the influence of a long incubation period of HLB in the plant. Motivated by the preceding discussion, our first aim of this paper is to formulate a mathematical model that is able to describe the dynamics of citrus HLB in citrus orchards, considering latent period as the time delay factor, and then to analyze the dynamic properties of the model.

    Disease management is complicated, because incubation periods are long and diagnosis is difficult. For the devastating citrus disease, the current state of preventive strategy involves insecticide spraying to reduce the abundance of psyllid vector population, removal of infected trees to reduce inoculum sources and nutrient solution injection to reduce the infection of the bacteria. There is an urgent need to find a sustainable and economical solution to the HLB menace through psyllid control by insecticides, removal of infected trees and nutrient solution injection. In recent years, using the Pontryagin's Maximum Principle to determine optimal control strategies for various diseases has flourished, see [16,17,18,19,20,21,22] and the references therein. For instance, the work by Lee et al. [18] introduced a dynamic model of pine nematode disease, in which nutrient injection, tree cutting, insecticide spraying and inhibition of mating of wood louse were used as control variables. In 2016, Pei et al. [22] established a delayed SIS model of infectious diseases with stage structure and introduced three treatment strategies into the model to study the existence and uniqueness of optimal control solution. But for the optimal control research of citrus HLB, there is few literatures (see [19,20]). In [19] and [20], although the authors considered different interventions for disease control, they did not take into account the time latency, which may lead to inappropriate policy making for preventing disease. Therefore, the second aim of this paper is to explore an optimal integrated strategy for a delayed HLB model considering the disease latency.

    The remaining of this paper is organized as follows. A model formulation is presented and the basic dynamics behavior of the model is analyzed in Section 2. Then sensitivity analysis is performed in Section 3. In Section 4, by using the results of the sensitivity analysis, an optimal control problem is developed, the optimal strategy is obtained and the uniqueness of the optimal control solution is proved. Numerical results with detailed discussions are presented in Section 5. Finally, this paper ends with a brief conclusion and the potential outlook for future work in Section 6.

    In this subsection, we will improve a HLB model taking the disease latency into account. Suppose that the citrus trees population totalling Nh consists of two categories that include the susceptible Sh and the infectious Ih. Additionally, the psyllids population, denoted by Nv, is divided into two classes, namely, susceptible Sv and infectious Iv.

    In order to better understand our model, the assumptions we made according to the transmission mechanism of HLB should be mentioned first of all:

    (A1): A susceptible citrus tree is assumed to become infected from contact with an infected psyllid with a probability of successful infection β, a susceptible psyllid becomes infected from contact with an infected tree, which happens at a probability α.

    (A2): All newly planted citrus trees are susceptible, moreover, new replanting has taken place at rate r with a proportion, KNh, of the orchard, where K represents the maximum capacity of citrus trees in the orchard. (A3): All newborn psyllids are susceptible, Λ is used to denote the constant recruitment rate of psyllid population.

    (A4): There is a 2 to 6 months latent period for susceptible citrus tree to have the capacity of contagiousness.

    Thus, a mathematical model considering latent period denoted by τ as the time delay factor can be formulated as follows:

    {dSh(t)dt=r(KNh(t))βSh(t)Iv(t)μhSh(t),dIh(t)dt=βSh(t)Iv(t)μhIh(t)γIh(t),dSv(t)dt=ΛαeμhτSv(t)Ih(tτ)μvSv(t),dIv(t)dt=αeμhτSv(t)Ih(tτ)μvIv(t), (2.1)

    where μh and μv are the natural mortality of citrus population and psyllid population, respectively. γ is the the disease-induced death rate of the infected trees. All parameters of model (2.1) are positive constants.

    Let C denote the Banach space of continuous functions ϕ : [τ,0]R4+ equipped with the sup-norm

    ϕ=supτθ0{|ϕ1(θ)|,|ϕ2(θ)|,|ϕ3(θ)|,|ϕ4(θ)|},

    here ϕ=(ϕ1,ϕ2,ϕ3,ϕ4)C([τ,0],R). Therefore, the initial condition for model (2.1) is taken as below:

    Sh(θ)=ϕ1(θ),Ih(θ)=ϕ2(θ),Sv(θ)=ϕ3(θ),Iv(θ)=ϕ4(θ)

    with

    ϕi(θ)0,θ[τ,0],ϕi(0)>0,i=1,2,3,4.

    Note that the citrus tree population Nh(t)=Sh(t)+Ih(t) and psyllid population Nv(t)=Sv(t)+Iv(t) satisfies

    ˙Nh(t)=rK(r+μh)Nh(t)γIh(t)rK(r+μh)Nh(t),˙Nv(t)=ΛμvNv(t),

    respectively, which implies that

    lim supt+Nh(t)=rKr+μh,limt+Nv(t)=Λμv.

    Define

    Ω={(Sh(t),Ih(t),Sv(t),Iv(t))R4+|0Sh(t)+Ih(t)rKr+μh,0Sv(t)+Iv(t)Λμv}.

    Obviously, Ω is a positively invariant set for system (2.1).

    As we all know, the basic reproductive number R0 is often considered as the threshold quantity that determines the dynamic behavior of the model. Following, we will calculate the basic reproductive number R0 of system (2.1) following the idea of [23].

    Suppose Ih(t)0, Iv(t)0, we can easily obtain the disease-free equilibrium, given by E0=(S0h,0,S0v,0), where S0h=rKr+μh,S0v=Λμv.

    Next, linearizing system (2.1) at the disease-free equilibrium E0 (here we only write down the equations of the diseased classes for simplification), this leads to

    {˙Ih(t)=βS0hIv(t)(μh+γ)Ih(t),˙Iv(t)=αeμhτS0vIh(tτ)μvIv(t).

    If we set Ih0, Iv0 be the numbers of each diseased class at time t=0, and Ih(t), Iv(t) be the remaining populations of each class at time t, respectively, then we have

    Ih(t)=Ih0e(μh+γ)t,Iv(t)=Iv0eμvt.

    Thus, the total numbers of newly infected in each diseased class can be expressed as

    ˉIh=0βS0hIv(t)dt=0βS0hIv0eμvtdt=βS0hμvIv0,ˉIv=ταeμhτS0vIh(tτ)dt=ταeμhτS0vIh0e(μh+γ)(tτ)dt=αeμhτS0vμh+γIh0.

    It then follows

    (ˉIhˉIv)=(0βS0hμvαeμhτS0vμh+γ0)(Ih0Iv0).

    Denote

    M=(0βS0hμvαeμhτS0vμh+γ0).

    We can see that M is the next infection operator, and the basic reproductive number, denoted by R0, can be described by the spectral radius of the matrix M. Therefore, R0 for system (2.1) is given by

    R0=Rvh×Rhv,

    where

    Rvh=βS0hμvandRhv=αeμhτS0vμh+γ.

    Qualitative analysis, including existence and stability are important topics in epidemic dynamics, we shall provide the stability analysis of equilibria for system (2.1) and look for the possibility of Hopf bifurcation by taking time delay "τ" as a bifurcation parameter in this subsection.

    When τ0, set the right-hand side of system (2.1) to zero, namely

    r(KShIh)βShIvμhSh=0,βShIv(μh+γ)Ih=0,ΛαeμhτSvIhμvSv=0,αeμhτSvIhμvIv=0. (2.2)

    So we have E=(Sh,Ih,Sv,Iv), where

    Sh=μv(μh+γ)αβeμhτSv,Ih=ΛμvSvαeμhτSv,Sv=Λβ(μh+γ+r)+μv(μh+r)(μh+γ)rKαβeμhτ+βμv(μh+γ+r),Iv=ΛμvSv.

    Obviously ΛμvSv>0 when R0>1, which leads to the existence of the unique endemic equilibrium.

    We have the following results on the stability of equilibria E0 and E by using the method in [24] when τ=0.

    Theorem 2.1. When τ=0, the disease-free equilibrium E0 of (2.1) is globally asymptotically stable if R0<1 and unstable if R0>1.

    Theorem 2.2. When τ=0, the endemic equilibrium E of (2.1) is locally asymptotically stable if R0>1.

    Now we turn to discussing the stability of the endemic equilibrium E when R0>1 in case of τ>0. In addition, we derive the stability conditions for E as well as the conditions for Hopf bifurcation.

    Linearizing system (2.1) at E, we get the following system

    ˙X=AX(t)+BX(tτ),

    where X=(Sh,Ih,Sv,Iv)T, A and B are 4×4 matrices, given by

    A=(rβIvμhr0βShβIvμhγ0βSh00αeμhτIhμv000αeμhτIhμv),
    B=(000000000αeμhτSv000αeμhτSv00).

    In view of |λIABeλτ|=0, we have

    |λ+r+βIv+μhr0βShβIvλ+μh+γ0βSh0αe(μh+λ)τSvλ+αeμhτIh+μv00αe(μh+λ)τSvαeμhτIhλ+μv|=0.

    It follows that

    λ4+b1λ3+b2λ2+b3λ+b4eλτ(c0λ2+c1λ)=0, (2.3)

    where

    b1=r+γ+2(μh+μv)+βIv+αeμhτIh,b2=(r+γ)(μh+2μv)+rγ+(μh+μv)2+2μhμv+βIv(r+γ+μh+2μv)+αeμhτIh(r+γ+2μh+μv)+βαeμhτIhIv,b3=2μv(r+μh)(γ+μh)+μ2v(2μh+r+γ)+βIvμv(2r+2γ+2μh+μv)+αeμhτIh[(r+μh)(γ+μh)+μv(r+γ+2μh)]+βαeμhτIhIv(r+γ+μh+μv),b4=μ2v(r+μh)(γ+μh)+μ2vβIv(r+γ+μh)+αeμhτIhμv(r+μh)(γ+μh)+βαeμhτIhIv(r+γ+μh),c0=βαeμhτShSv,c1=βαeμhτShSv(r+μh).

    To show Hopf bifurcation, we must have a pair of purely imaginary roots of characteristic Eq (2.3). Suppose iω(ω>0) is a purely imaginary root associated with Eq (2.3), thus

    ω4ib1ω3b2ω2+ib3ω+b4=c0ω2cosωτ+ic1ωcosωτ+ic0ω2sinωτ+c1ωsinωτ.

    Separating real and imaginary parts, we have following equations

    ω4b2ω2+b4=c0ω2cosωτ+c1ωsinωτ, (2.4)
    b1ω3+b3ω=c1ωcosωτ+c0ω2sinωτ. (2.5)

    Squaring and adding (2.4) and (2.5) we obtain

    ω8+(b212b2)ω6+(b22+2b42b1b3c20)ω4+(b232b2b4c21)ω2+b24=0. (2.6)

    Let z=ω2, then Eq (2.6) yields

    f(z)=z4+q1z3+q2z2+q3z+q4=0, (2.7)

    where the coefficients are given by

    q1=b212b2,q2=b22+2b42b1b3c20,q3=b232b2b4c21,q4=b24.

    Now, if the following conditions q10, q20, q3>0, q40 are satisfied, then there will be no positive roots of Eq (2.7), which implies there is no any purely imaginary roots of characteristic Eq (2.3). In the case for τ0 all characteristic roots of Eq (2.3) have negative real part by Rouchet theorem [25]. Hence, the following result is claimed.

    Theorem 2.3. If the conditions R0>1, q10, q20, q3>0 and q40 are satisfied, then the endemic equilibrium E of system (2.1) is local asymptotically stable for all τ0.

    However, if the coefficients of Eq (2.7) satisfy q10, q20, q30, q4<0, then Eq (2.7) has at least one positive real root. It means that Eq (2.6) has at least one positive real root for z=ω2.

    Let ω0 be a positive real root of Eq (2.6). Then there is a purely imaginary root iω0 of Eq (2.3). From Eqs (2.4) and (2.5) we obtain the values of cosωτ as

    cosωτ=c0ω2(ω4b2ω2+b4)+c1ω(b3ωb1ω3)c20ω4+c21ω2. (2.8)

    Furthermore, substituting ω=ω0 into (2.8), then delay factor τ can be presented

    τk=1ω0arccos(c0ω20(ω40b2ω20+b4)+c1ω0(b3ω0b1ω30)c20ω40+c21ω20)+2kπω0,k=0,1,2,. (2.9)

    Hence (ω0,τk) is the solution of Eq (2.3), that is to say, there exists a pair of purely imaginary roots λ=±iω0 for Eq (2.3) when τ=τk.

    Note that τ=τ0 is the minimum value of τ when the purely imaginary root λ=±iω0 of Eq (2.3) occurs. Based on above discussion, we state following lemmas which will be essential to our claims.

    Lemma 2.1. Eq (2.3) has a pair of purely imaginary roots λ=±iω0 if q10, q20, q30, q4<0, τ=τ0.

    Set the characteristic value of Eq (2.3) to be λ(τ)=α(τ)+iω(τ) satifying the condition of α(τk)=0 and ω(τk)=ω0, the transversality condition is verified below.

    Lemma 2.2. If the condition f(ω20)=4ω60+3q1ω40+2q2ω20+q30 holds, then dReλ(τ)dττ=τk0.

    Proof. Differentiating both sides of Eq (2.3) with respect to τ, we have

    (4λ3+3b1λ2+2b2λ+b3)dλdτ=[τeλτ(c0λ2+c1λ)+eλτ(2c0λ+c1)]dλdτλeλτ(c0λ2+c1λ).

    Obviously,

    (dλdτ)1=4λ3+3b1λ2+2b2λ+b3+τeλτ(c0λ2+c1λ)eλτ(2c0λ+c1)λeλτ(c0λ2+c1λ)=4λ3+3b1λ2+2b2λ+b3λeλτ(c0λ2+c1λ)+2c0λ+c1λ(c0λ2+c1λ)τλ=4λ3+3b1λ2+2b2λ+b3λ(λ4+b1λ3+b2λ2+b3λ+b4)+2c0λ+c1λ(c0λ2+c1λ)τλ. (2.10)

    It follows from λ(τk)=iω0 and (2.10) that

    Re[(dλdτ)1|τ=τk]=Re[4λ3+3b1λ2+2b2λ+b3λ(λ4+b1λ3+b2λ2+b3λ+b4)|τ=τk]+Re[2c0λ+c1λ(c0λ2+c1λ)|τ=τk]=Re[4iω303b1ω20+2b2iω0+b3iω0(ω40b1iω30b2ω2+b3iω0+b4)]+Re[2c0iω0+c1iω0(c0ω20+c1iω0)]=ω20[4ω60+3(b212b2)ω402(2b1b32b4b22)ω20+b232b2b4](b3ω20b1ω40)2+(ω50b2ω30+b4ω0)2+c21ω202c20ω40(c1ω20)2+(c0ω30)2=4ω60+3(b212b2)ω402(2b1b32b4b22)ω20+b232b2b4(b3ω0b1ω30)2+(ω40b2ω20+b4)2+c212c20ω20(c1ω0)2+(c0ω20)2. (2.11)

    After substituting λ=iω0 into Eq (2.3) we can see that

    ω40b1iω30b2ω20+b3iω0+b4(c0ω20+c1iω0)eiω0τ=0. (2.12)

    Considering |eiω0τ|=1 for eiω0τ=cosω0τisinω0τ, we derive from (2.12) that

    |ω40b2ω20+b4(b1ω30b3ω0)i|=|c0ω20+c1ω0i|.

    Consequently,

    (ω40b2ω20+b4)2+(b1ω30b3ω0)2=(c0ω20)2+(c1ω0)2. (2.13)

    Finally, from (2.11) and (2.13) we get

    Re[(dλdτ)1|τ=τk]=4ω60+3(b212b2)ω40+2(b22+2b42b1b3c20)ω20+b232b2b4c21(c0ω20)2+(c1ω0)2=4ω60+3q1ω40+2q2ω20+q3(c0ω20)2+(c1ω0)2=f(ω20)(c0ω20)2+(c1ω0)20.

    This completes the proof.

    Therefore, based on Hopf bifurcation theory and the above discussions we have the following theorem.

    Theorem 2.4. If the conditions q10, q20, q30, q4<0, f(ω20)0 and R0>1 hold, then the endemic equilibrium E of system (2.1) is asymptotically stable for τ<τ0; the endemic equilibrium E of system (2.1) is unstable for τ>τ0; Hopf bifurcation occurs at E for τ=τk(k=0,1,2,).

    Uncertainty analyses and sensitivity analyses are necessary to explore the behavior of many complex models, because the structural complexity of the models are coupled with a high degree of uncertainty in estimating the values of many of the input parameter [26]. In this section, we employed a global sensitivity analysis to assess the impact of uncertainty and the sensitivity of the outcomes of the numerical simulations to variations in each parameter of model (2.1) using Latin Hypercube Sampling (LHS) and partial rank correlation coefficient (PRCC). LHS is a stratified sampling without replacement technique which allows for an efficient analysis of parameter variations across simultaneous uncertainty ranges in each parameter [26,27,28,29]. Further, PRCC is used to measure the strength of the relationship between the model outcome and the parameters, state the degree of the effect that each parameter has on the outcome [26,27,28,29]. Therefore, by sensitivity analyses we can assess the parameters with the most significant impact on the outcome of the numerical simulations of the model.

    Initial disease transmission is directly related to the reproductive number R0, it is a combination of parameters related to both the trees and the psyllids. Therefore, in determining the control measure which is the most effective in controlling HLB transmission, we use R0 as the response function. Firstly, we calculate the sensitivity indices of R0 to the parameters in the model. These indices tell us how crucial each parameter is to disease transmission and prevalence. All numerical parameter values of model (2.1) are presented in Table 1.

    Table 1.  Parameters in the model (2.1) for transmission dynamics of citrus Huanglongbing.
    Parameter Estimated value Unit Reference
    r 0.5 - Assume
    K 2000 - [31]
    α 3.26×105 month1 [32]
    β 4.07×105 month1 [32]
    γ 0.05 month1 [1]
    Λ 27710 month1 [32]
    μh 0.0033 month1 [33]
    μv 0.5 month1 [32]
    τ 6 month [34]

     | Show Table
    DownLoad: CSV

    Definition 3.1. [30] The normalized forward sensitivity index of a variable, u, that depends differentially on a parameter, p, is defined as:

    γup:=up×pu. (3.1)

    Then we derive an analytical expression for the sensitivity of R0,

    γR0p=R0p×pR0, (3.2)

    to each of the nine different parameters described in Table 2. For example, the sensitivity index of R0 with respect to β,

    γR0β=R0β×βR0=0.5, (3.3)
    Table 2.  Sensitivity index of R0.
    Parameter Description Sensitivity index
    α Infection rate from infected citrus trees to susceptible citrus psyllid 0.5
    β Infection rate from infected citrus psyllid to susceptible citrus trees 0.5
    K Maximum citrus population size 0.5
    Λ Constant recruitment rate of psyllid population 0.5
    r The replanted rate of citrus trees 0.0033
    μv Natural death rate of citrus psyllid -1
    μh Natural death rate of citrus trees -0.0715
    γ Disease-induced mortality of the infected trees -0.4417
    τ Latent period -0.0099

     | Show Table
    DownLoad: CSV

    does not depend on any parameter values.

    It follows from Table 2 that the most sensitive parameter is the natural death rate of citrus psyllid, μv. Other important parameters include infection rate from infected citrus trees to susceptible citrus psyllid, α, the infection rate from infected citrus psyllid to susceptible citrus trees, β, and the disease-induced mortality of the infected trees, γ. Since γR0β=0.5, decreasing (or increasing) β by 10% increases (or decreases) R0 by 5%. Similarly, as γR0γ=0.4417, increasing (or decreasing) γ by 10% decreases (or increases) R0 by 4.417%.

    Next, we use sensitivity analysis to discover parameters that have a high impact on the basic reproductive number R0, and should be targeted by intervention strategies. Figure 1 presents our sensitivity analysis on R0, which involved computing the PRCC of R0 using the LHS method. We see from Figure 1 that the natural mortality of psyllid population μv has the most effect on R0 of all the constant parameters. This occurs because the parameter is involved in both directions of transmission: from a tree to a psyllid and vice versa. In addition, we can see that the parameters α, β, Λ, r and K have the positive impact on R0. For example, a decrease in β decreases R0, whereas other parameters (i.e., μh, μv, γ, τ) are negatively correlated with R0.

    Figure 1.  Sensitivity analysis of the basic reproduction number R0.

    Identification of these key parameters is important to the formulation of effective control strategies necessary for reducing the prevalence of the disease in the grove. In particular, the results of this sensitivity analysis suggest that a strategy that reduces the parameters with positive impact on R0 will adequately reduce the spread of HLB in the grove. Furthermore, a strategy that increases the parameters with negative impact on R0 will be effective in curtailing the spread of HLB in the grove.

    Therefore, it follows from sensitivity analysis that the disease in the grove can be effectively reduced using control strategies:

    Nutrient solution injecting u1(t) (i.e., decrease the value of the parameter β);

    Infected trees removal u2(t) (i.e., increase the value of the parameter γ);

    Insecticides spraying u3(t) (i.e., increase the value of the parameter μv).

    The results of the sensitivity analysis suggest that control strategies that reduce infection rate (β), increase disease-induced mortality of the infected trees (γ) and psyllid natural death rate (μv) will be effective in curtailing the spread of HLB in the grove. However, large quantities use of insecticides and removal of infected trees in large numbers have been associated with the increased cost, which is an important problem in sustainable control of HLB. For this, there is an urgent need to find an optimal control strategy in terms of possible combination of strategies to prevent the spread of citrus HLB while minimizing the implementation cost. In this section, we suggest the following delayed control system with three-time-dependent control variables u1(t), u2(t), and u3(t):

    {dSh(t)dt=r(KNh(t))β(1ς1u1(t))Sh(t)Iv(t)μhSh(t),dIh(t)dt=β(1ς1u1(t))Sh(t)Iv(t)μhIh(t)γIh(t)ς2u2(t)Ih(t),dSv(t)dt=ΛαeμhτSv(t)Ih(tτ)μvSv(t)ς3u3(t)Sv(t),dIv(t)dt=αeμhτSv(t)Ih(tτ)μvIv(t)ς3u3(t)Iv(t), (4.1)

    with the initial conditions

    Sh(t)=Sh0,Ih(t)=Ih0,Sv(t)=Sv0,Iv(t)=Iv0,ui(t)=ui0,forτt0, (4.2)

    where ς1, ς2 and ς3 denote the maximum injecting rate of nutrient solution, removing rate and killing rate, respectively, and the control functions u(t)=(u1(t),u2(t),u3(t)) belong to the control set U defined by

    U={(u1,u2,u3):ui is Lebsegue measurable,0ui(t)1,t[0,T],i=1,2,3}. (4.3)

    Here T is the control period.

    For the optimal control problem of system (4.1), we now consider the following objective functional

    J(u1,u2,u3)=T0(A1Ih(t)+A2Iv(t)+B12u21(t)+B22u22(t)+B32u23(t))dt. (4.4)

    Generally, cost function for each control is assumed to be quadratic. The parameters A1, A2 and B1, B2, B3 represent the desired weights on the benefit and cost. The objective functional J formulates the optimization problem of identifying the most effective strategies, which involves the minimization of the number of the infected citrus trees and psyllids and total implementation cost over a finite time interval [0,T]. The goal of the optimal control problem is to seek an optimal control (u1,u2,u3) such that

    J(u1,u2,u3)=minUJ(u1,u2,u3),

    where the control set U is defined in (4.3) and subject to control system (4.1) with initial conditions (4.2).

    In what follows, we use Pontryagin's Maximum Principle [35] to solve this optimal control problem with time delay.

    Note that non-negative bounded solutions to the state system exists for the bounded Lebesgue measurable controls and non-negative initial conditions. We assume not only the control variables u1(t), u2(t) and u3(t) satisfy constraints (4.3) but also Sh(θ),Ih(θ),Sv(θ),Iv(θ) are non-negative continuous functions for θ[τ,0] and

    Sh(0)=Sh0>0,Ih(0)=Ih0,Sv(0)=Sv0>0,Iv(t)=Iv0.

    Then system (4.1) can be rewritten in matrix form as follows:

    ˙V(t)=AV(t)+F(V(t),Vτ(t))+C(u,V(t)), (4.5)

    where

    ˙V(t)=(˙Sh(t)˙Ih(t)˙Sv(t)˙Iv(t)),
    F(V(t),Vτ(t))=(rKβSh(t)Iv(t)βSh(t)Iv(t)ΛαeμhτSv(t)Ih(tτ)αeμhτSv(t)Ih(tτ)), (4.6)
    A=(rμhr000μhγ0000μv0000μv),
    C(u,V(t))=(βς1u1(t)Sh(t)Iv(t)βς1u1(t)Sh(t)Iv(t)ς2u2(t)Ih(t)ς3u3(t)Sv(t)ς3u3(t)Iv(t)),

    and Vτ(t)=V(tτ). It is easy to see that system (4.1) is a nonlinear system with bounded coefficients.

    Denote

    G(V(t),Vτ(t))=AV(t)+F(V(t),Vτ(t)), (4.7)

    and

    |V1(t)V2(t)||Sh1(t)Sh2(t)|+|Ih1(t)Ih2(t)|+|Sv1(t)Sv2(t)|+|Iv1(t)Iv2(t)|,
    |(V1)τ(t)(V2)τ(t)||(Sh1)τ(t)(Sh2)τ(t)|+|(Ih1)τ(t)(Ih2)τ(t)|+|(Sv1)τ(t)(Sv2)τ(t)|+|(Iv1)τ(t)(Iv2)τ(t)|,

    here,

    (Shi)τ(t)=Shi(tτ),(Ihi)τ(t)=Ihi(tτ),(Svi)τ(t)=Svi(tτ),(Ivi)τ(t)=Ivi(tτ),i=1,2.

    It then follows from (4.6) that there exist positive constants L1 and L2 such that

    |F(V1(t),(V1)τ(t))F(V2(t),(V2)τ(t))|L1|V1(t)V2(t)|+L2|(V1)τ(t)(V2)τ(t)|,

    where L1 and L2 are independent of state variables Sh(t), Ih(t), Sv(t) and Iv(t).

    Consequently, we obtain

    |G(V1,V1τ)G(V2,V2τ)|L(|V1(t)V2(t)|+|(V1)τ(t)(V2)τ(t)|),

    where L=max{L1,L2,A}<, which shows that G is uniformly Lipschitz continuous, hence by definition of U with the restriction on Sh(t), Ih(t), Sv(t), Iv(t)0, we can see that the solution of system (4.1) exists following the Theorem 4.1 and its corresponding corollary by Fleming and Rishel [36].

    Theorem 4.1. There exists an optimal control (u1,u2,u3)U such that

    J(u1,u2,u3)=minUJ(u1,u2,u3),

    subject to the control system (4.1) with the initial conditions (4.2).

    Proof. The existence of an optimal control problem can be verified by using the result in [36]. It is obvious to see that both the control variables and the state variables are non-negative values, which satisfies the necessary convexity of the objective functional. Note that the set of all the control variables (u1(t),u2(t),u3(t))U is convex and closed by definition. The optimal system is bounded which determines the compactness needed for the existence of the optimal control. Also, the integrand in the functional (4.4), i.e., A1Ih+A2Iv+B12u21+B22u22+B32u23, is convex on the control set U. Besides, we can see that, there exists constants η1, η2>0 and ρ>1 such that

    A1Ih(t)+A2Iv(t)+B12u21(t)+B22u22(t)+B32u23(t)η1(|u1|2+|u2|2+|u3|2)ρ/2η2,

    which completes the existence of an optimal control.

    Based on the well-known technique Pontryagin's Maximum Principle, we manage to obtain the optimal solution of the control system (4.1). For convenience, we set:

    X(t)=(Sh(t),Ih(t),Sv(t),Iv(t)),Xτ(t)=(Shτ(t),Ihτ(t),Svτ(t),Ivτ(t)),Shτ(t)=Sh(tτ),Ihτ(t)=Ih(tτ),Svτ(t)=Sv(tτ),Ivτ(t)=Iv(tτ),u=(u1(t),u2(t),u3(t)),λ(t)=(λ1(t),λ2(t),λ3(t),λ4(t)).

    To determine the precise formulation of our optimal control, we consider the optimal control problem (4.1)-(4.4) to find the Lagrangian function as well as Hamiltonian function. The Lagrangian function L is given by

    L(X,u)=A1Ih(t)+A2Iv(t)+B12u21(t)+B22u22(t)+B32u23(t),

    and the Hamiltonian function H is

    H(X,Xτ,u,λ)=A1Ih(t)+A2Iv(t)+B12u21(t)+B22u22(t)+B32u23(t)+λ1(t)(r(KNh(t))β(1ς1u1(t))Sh(t)Iv(t)μhSh(t))+λ2(t)(β(1ς1u1(t))Sh(t)Iv(t)μhIh(t)γIh(t)ς2u2(t)Ih(t))+λ3(t)(ΛαeμhτSv(t)Ih(tτ)μvSv(t)ς3u3(t)Sv(t))+λ4(t)(αeμhτSv(t)Ih(tτ)μvIv(t)ς3u3(t)Iv(t)), (4.8)

    where λ1(t), λ2(t), λ3(t) and λ4(t) are the adjoint variables.

    For simplicity, we introduce a indicative function

    χ[0,Tτ](t)={1if0tTτ,0ifTτtT. (4.9)

    Notice that a necessary condition for optimality problems can be found in [35]. If we consider X(t) and Xτ(t) defined above, then there exists a continuous function λ(t) on [0,T] satisfying equations given below, namely, the state equations

    ˙X(t)=Hλ(X,Xτ,u,λ)(t), (4.10)

    the optimal condition

    0=Hu(X,Xτ,u,λ)(t), (4.11)

    and the adjoint equation

    ˙λ(t)=HX(X,Xτ,u,λ)(t)+χ[0,Tτ](t)HXτ(X,Xτ,u,λ)(t)|(t+τ), (4.12)

    where Hλ, Hu, HX and HXτ denote the derivatives of the Hamiltonian H with respect to λ, u, X and Xτ, respectively. Now, applying the necessary condition to Hamiltonian H in (4.8) with X=X, following result hence obtain.

    Theorem 4.2. Let X=(Sh, Ih, Sv, Iv) be an optimal state solution associated with the optimal control variable u=(u1, u2, u3) for the optimal control problem (4.1)-(4.4). Then there exist four adjoint variables λi(t),(i=1,2,3,4) satisfying the adjoint equations as follows

    {˙λ1(t)=λ1(t)(rβ(1ς1u1(t))Iv(t)μh)λ2(t)β(1ς1u1(t))Iv(t),˙λ2(t)=A1+λ1(t)rλ2(t)(μhγς2u2(t))χ[0,Tτ](t)[λ3(t+τ)(αeμhτSv(t+τ))+λ4(t+τ)αeμhτSv(t+τ)],˙λ3(t)=λ3(t)(αeμhτIh(tτ)μvς3u3(t))λ4(t)αeμhτIh(tτ),˙λ4(t)=A2λ1(t)(β(1ς1u1(t))Sh(t))λ2(t)β(1ς1u1(t))Sh(t)λ4(t)(μvς3u3(t)), (4.13)

    with transversality conditions

    λi(T)=0,i=1,2,3,4. (4.14)

    Moreover, the optimal controls u1, u2 and u3 are characterized in the following

    u1=max{min{(ς2λ2(t)ς1λ1(t))βSh(t)Iv(t)B1,1},0},u2=max{min{ς2λ2(t)Ih(t)B2,1},0},u3=max{min{ς3(λ3(t)Sv(t)+λ4(t)Iv(t))B3,1},0}. (4.15)

    Proof. The proof follows from Pontryagin's Maximum Principle. By using the adjoint equation (4.12) and differentiating the Hamiltonian (4.8) with respect to X(t)=X(t) and Xτ(t)=Xτ(t), we obtain

    ˙λ1(t)=HSh(t)+χ[0,Tτ](t)HShτ(t)(t+τ),˙λ2(t)=HIh(t)+χ[0,Tτ](t)HIhτ(t)(t+τ),˙λ3(t)=HSv(t)+χ[0,Tτ](t)HSvτ(t)(t+τ),˙λ4(t)=HIv(t)+χ[0,Tτ](t)HIvτ(t)(t+τ). (4.16)

    Then substituting the corresponding derivatives HX(t) and HXτ(t) (here X=Sh,Ih,Sv,Iv) into (4.16), we can obtain the adjoint equations (4.13). Further, from the optimal conditions (4.11), we have

    Hu1=B1u1+λ1(t)βς1Sh(t)Iv(t)λ2(t)βς2Sh(t)Iv(t)=0,Hu2=B2u2λ2(t)ς2Ih(t)=0,Hu3=B3u3λ3(t)ς3Sv(t)λ4(t)ς3Iv(t)=0,

    which indicates

    u1=(ς2λ2(t)ς1λ1(t))βSh(t)Iv(t)B1,u2=ς2λ2(t)Ih(t)B2,u3=ς3(λ3(t)Sv(t)+λ4(t)Iv(t))B3.

    Taking into account the property of control set in (4.3), we obtain

    u1(t)={0if(ς2λ2(t)ς1λ1(t))βSh(t)Iv(t)B10,(ς2λ2(t)ς1λ1(t))βSh(t)Iv(t)B1if0<(ς2λ2(t)ς1λ1(t))βSh(t)Iv(t)B1<1,1if(ς2λ2(t)ς1λ1(t))βSh(t)Iv(t)B11,
    u2(t)={0ifς2λ2(t)Ih(t)B20,ς2λ2(t)Ih(t)B2if0<ς2λ2(t)Ih(t)B2<1,1ifς2λ2(t)Ih(t)B21,
    u3(t)={0ifς3(λ3(t)Sv(t)+λ4(t)Iv(t))B30,ς3(λ3(t)Sv(t)+λ4(t)Iv(t))B3if0<ς3(λ3(t)Sv(t)+λ4(t)Iv(t))B3<1,1ifς3(λ3(t)Sv(t)+λ4(t)Iv(t))B31,

    This can be rewritten in compact notations:

    u1=max{min{(ς2λ2(t)ς1λ1(t))βSh(t)Iv(t)B1,1},0},u2=max{min{ς2λ2(t)Ih(t)B2,1},0},u3=max{min{ς3(λ3(t)Sv(t)+λ4(t)Iv(t))B3,1},0}.

    This completes our proof.

    Formulae represented in (4.15) are the characterization of the optimal controls. In addition, the second derivative of the Lagrangian L with respect to u1(t), u2(t) and u3(t) is positive, which shows that the optimal problem is minimum at controls u1(t), u2(t) and u3(t). Further, the optimality system, which consists of the adjoint equations (4.13) and the state equations (4.1), the transversality conditions (4.14) with the explicit representations (4.15) for the controls is given below.

    {˙Sh(t)=r(KNh(t))β(1ς1max{min{(ς2λ2(t)ς1λ1(t))βSh(t)Iv(t)B1,1},0})×Sh(t)Iv(t)μhSh(t),˙Ih(t)=β(1ς1max{min{(ς2λ2(t)ς1λ1(t))βSh(t)Iv(t)B1,1},0})Sh(t)Iv(t)μhIh(t)γIh(t)ς2max{min{ς2λ2(t)Ih(t)B2,1},0}Ih(t),˙Sv(t)=ΛαeμhτSv(t)Ih(tτ)μvSv(t)ς3max{min{ς3(λ3(t)Sv(t)+λ4(t)Iv(t))B3,1},0}Sv(t),˙Iv(t)=αeμhτSv(t)Ih(tτ)μvIv(t)ς3max{min{ς3(λ3(t)Sv(t)+λ4(t)Iv(t))B3,1},0}Iv(t),˙λ1(t)=λ1(t)(rβ(1ς1max{min{(ς2λ2(t)ς1λ1(t))βSh(t)Iv(t)B1,1},0})Iv(t)μh)λ2(t)β(1ς1max{min{(ς2λ2(t)ς1λ1(t))βSh(t)Iv(t)B1,1},0})Iv(t),˙λ2(t)=A1+λ1(t)rλ2(t)(μhγς2max{min{ς2λ2(t)Ih(t)B2,1},0})χ[0,Tτ](t)[λ3(t+τ)(αeμhτSv(t+τ))+λ4(t+τ)αeμhτSv(t+τ)],˙λ3(t)=λ3(t)(αeμhτIh(tτ)μvς3max{min{ς3(λ3(t)Sv(t)+λ4(t)Iv(t))B3,1},0})λ4(t)αeμhτIh(tτ),˙λ4(t)=A2λ1(t)(β(1ς1max{min{(ς2λ2(t)ς1λ1(t))βSh(t)Iv(t)B1,1},0})×Sh(t))λ2(t)β(1ς1max{min{(ς2λ2(t)ς1λ1(t))βSh(t)Iv(t)B1,1},0})Sh(t)λ4(t)(μvς3max{min{ς3(λ3(t)Sv(t)+λ4(t)Iv(t))B3,1},0}), (4.17)

    with initial conditions (4.2) and transversality conditions (4.14).

    The optimal control depends on adjoint variables and state variables, thus the uniqueness of the optimal control derives from the uniqueness of the optimality system. In this subsection, we attempt to prove that the optimal system has a unique solution. Note that Sh(t), Ih(t), Sv(t), Iv(t) are bounded, then the adjoint equation (4.13) has a bounded right-hand side which is dependent on the final time T. Therefore, there exists a positive constant M, which is dependent on the coefficients of the state equation and the uniform bound for Sh(t), Ih(t), Sv(t) and Iv(t) such that λi∣<MT on [0,T].

    Theorem 4.3. For T sufficiently small, the solution to the optimality system (4.17) is unique.

    Proof. Suppose that (Sh,Ih,Sv,Iv) and (¯Sh,¯Ih,¯Sv,¯Iv) are two distinct solutions to the optimality system (4.17). Let m0>0 be chosen such that

    Sh=em0th,Ih=em0tq,Sv=em0tf,Iv=em0tl,λ1=em0tω,λ2=em0tυ,λ3=em0tj,λ4=em0tk, (4.18)
    ¯Sh=em0t¯h,¯Ih=em0t¯q,¯Sv=em0t¯f,¯Iv=em0t¯l,¯λ1=em0t¯ω,¯λ2=em0t¯υ,¯λ3=em0t¯j,¯λ4=em0t¯k. (4.19)

    It follows from (4.15), (4.18) and (4.19) that

    u1=max{min{(ς2υς1ω)βhlem0tB1,1},0},u2=max{min{ς2υqB2,1},0},u3=max{min{ς3(jf+kl)B3,1},0}, (4.20)
    ¯u1=max{min{(ς2¯υς1¯ω)β¯h¯lem0tB1,1},0},¯u2=max{min{ς2¯υ¯qB2,1},0},¯u3=max{min{ς3(¯j¯f+¯k¯l)B3,1},0}. (4.21)

    Denote

    Q=T0(hˉh)2+(qˉq)2+(fˉf)2+(lˉl)2+(ωˉω)2+(vˉv)2+(jˉj)2+(kˉk)2dt.

    To prove our main result, we firstly show the following two claims are valid.

    Claim I . There exist positive constants Cx and Dx such that

    12[(x(0)ˉx(0))2]+axT0(xˉx)2dtCxQ+Dxem0TQ

    holds, where x=ω,v,j,k, and aω=m0+r+μh, av=m0+μh+γ, aj=m0+μv, ak=m0+μv.

    Without loss of generality, we take x=v to analyze. Other cases can be discussed similarly. Substituting (4.18)-(4.21) into the sixth equation of system (4.17), we have

    m0v+v=A1em0t+rω+(μh+γ)v+ς2vmax{min{ς2vqB2,1},0}+χ[0,Tτ](t)em0tμhταf(t+τ)j(t+τ)χ[0,Tτ](t)em0tμhταf(t+τ)k(t+τ),

    and

    m0ˉv+ˉv=A1em0t+rˉω+(μh+γ)ˉv+ς2ˉvmax{min{ς2ˉvˉqB2,1},0}+χ[0,Tτ](t)em0tμhταˉf(t+τ)ˉj(t+τ)χ[0,Tτ](t)em0tμhταˉf(t+τ)ˉk(t+τ).

    Subtracting the above two equations, we have

    (m0+μh+γ)(vˉv)(vˉv)=r(ˉωω)+ς2ˉvmax{min{ς2¯v¯qB2,1},0}ς2vmax{min{ς2vqB2,1},0}+χ[0,Tτ](t)em0tμhτα(ˉf(t+τ)ˉj(t+τ)f(t+τ)j(t+τ))+χ[0,Tτ](t)em0tμhτα(f(t+τ)k(t+τ)ˉf(t+τ)ˉk(t+τ)). (4.22)

    Multiplying (4.22) by vˉv and then integrating from 0 to T, we can derive the following equality by transversality conditions (4.14).

    T0(m0+μh+γ)(vˉv)2dtT0(vˉv)(vˉv)dt=(m0+μh+γ)T0(vˉv)2dt+12[(v(0)ˉv(0))2]. (4.23)

    From (4.22) and (4.23), we get

    12[(v(0)ˉv(0))2]+(m0+μh+γ)T0(vˉv)2dt=T0r(ˉωω)(vˉv)dt+T0ς2(ˉvmax{min{ς2¯v¯qB2,1},0}vmax{min{ς2vqB2,1},0})(vˉv)dt+T0χ[0,Tτ](t)em0tμhτα(ˉf(t+τ)ˉj(t+τ)f(t+τ)j(t+τ))(vˉv)dt+T0χ[0,Tτ](t)em0tμhτα(f(t+τ)k(t+τ)ˉf(t+τ)ˉk(t+τ))(vˉv)dt. (4.24)

    Note that em0tμhτ<em0T, 0<χ[0,Tτ](t)<1 for 0<t<T, (4.24) yields

    12[(v(0)ˉv(0))2]+(m0+μh+γ)T0(vˉv)2dtT0r(ˉωω)(vˉv)dt+T0ς2(ˉvmax{min{ς2¯v¯qB2,1},0}vmax{min{ς2vqB2,1},0})(vˉv)dt+αem0TT0χ[0,Tτ](t)(ˉf(t+τ)ˉj(t+τ)f(t+τ)j(t+τ))(vˉv)dt+αem0TT0χ[0,Tτ](t)(f(t+τ)k(t+τ)ˉf(t+τ)ˉk(t+τ))(vˉv)dt.I1+I2+αem0TI3+αem0TI4, (4.25)

    where

    I1=T0r(ˉωω)(vˉv)dt,I2=T0ς2(ˉvmax{min{ς2¯v¯qB2,1},0}vmax{min{ς2vqB2,1},0})(vˉv)dt,I3=T0χ[0,Tτ](t)(ˉf(t+τ)ˉj(t+τ)f(t+τ)j(t+τ))(vˉv)dt,I4=T0χ[0,Tτ](t)(f(t+τ)k(t+τ)ˉf(t+τ)ˉk(t+τ))(vˉv)dt.

    In the following, we will calculate formulae I1-I4 and enlarge them into the form of sum of squares by using the inequality ab(a2+b2)/2. It is obvious to show that

    I1=T0r(ˉωω)(vˉv)dtrT0(ωˉω)2+(vˉv)2dt. (4.26)

    Besides, we can see that there exists a positive constant M1 such that

    I2=T0ς2(ˉvmax{min{ς2¯v¯qB2,1},0}vmax{min{ς2vqB2,1},0})(vˉv)dt=T0ς2(ˉv(max{min{ς2¯v¯qB2,1},0}max{min{ς2vqB2,1},0})+max{min{ς2vqB2,1},0}(ˉvv))(vˉv)dtT0ς2(ς2ˉvB2|ˉvˉqvq|+|vˉv|)(vˉv)dtT0ς2(ς2ˉv2B2|ˉqq|+|ς2ˉvqB2+1||vˉv|)(vˉv)dtM1T0(qˉq)2+(vˉv)2dt. (4.27)

    Next we will specifically analyze formula I3. In view of ˉf(t+τ)ˉj(t+τ)f(t+τ)j(t+τ)=ˉf(t+τ)ˉj(t+τ)ˉf(t+τ)j(t+τ)+ˉf(t+τ)j(t+τ)f(t+τ)j(t+τ), we have

    I3=T0χ[0,Tτ](t)(ˉf(t+τ)ˉj(t+τ)f(t+τ)j(t+τ))(vˉv)dt=T0χ[0,Tτ](t)(ˉf(t+τ)ˉj(t+τ)ˉf(t+τ)j(t+τ)+ˉf(t+τ)j(t+τ)f(t+τ)j(t+τ))(vˉv)dt=T0χ[0,Tτ](t)[(vˉv)ˉf(t+τ)(ˉj(t+τ)j(t+τ))+(vˉv)j(t+τ)(ˉf(t+τ)f(t+τ))]dt.M2T0χ[0,Tτ](t)(vˉv)(ˉj(t+τ)j(t+τ))dt+M3T0χ[0,Tτ](t)(vˉv)(ˉf(t+τ)f(t+τ))dt, (4.28)

    where M2, M3 are the upper bounds for ˉf(t+τ) and j(t+τ), respectively.

    Further, by using the inequality ab(a2+b2)/2, we have

    T0χ[0,Tτ](t)(vˉv)(ˉj(t+τ)j(t+τ))dtT0(vˉv)2dt+T0χ[0,Tτ](t)(ˉj(t+τ)j(t+τ))2dt,=T0(vˉv)2dt+Tτ0(ˉj(t+τ)j(t+τ))2dt=T0(vˉv)2dt+Tτ(ˉj(t)j(t))2dtT0(vˉv)2dt+T0(j(t)ˉj(t))2dt. (4.29)

    By similar above discussion, we can yield

    T0χ[0,Tτ](t)(vˉv)(ˉf(t+τ)f(t+τ))dtT0(vˉv)2dt+T0(fˉf)2dt. (4.30)

    It follows from (4.28), (4.29) and (4.30) that

    I3M2T0(vˉv)2+(jˉj)2dt+M3T0(vˉv)2+(fˉf)2dt. (4.31)

    Similarly, we can obtain that there exist positive constants M4 and M5 such that

    I4=T0χ[0,Tτ](t)(f(t+τ)k(t+τ)ˉf(t+τ)ˉk(t+τ))(vˉv)dtM4T0(vˉv)2+(kˉk)2dt+M5T0(vˉv)2+(fˉf)2dt. (4.32)

    From (4.26), (4.27), (4.31) and (4.32), we can conclude

    12[(v(0)ˉv(0))2]+(m0+μh+γ)T0(vˉv)2dtrT0(ωˉω)2+(vˉv)2dt+M1T0(qˉq)2+(vˉv)2dt+max{M2,M3}αem0T(T0(fˉf)2+(vˉv)2+(jˉj)2dt)+max{M4,M5}αem0T(T0(fˉf)2+(vˉv)2+(kˉk)2dt)Cv[T0(qˉq)2+(ωˉω)2+(vˉv)2dt]+Dvem0T[T0(fˉf)2+(vˉv)2+(jˉj)2+(kˉk)2dt].CvQ+Dvem0TQ.

    Claim II . There exist positive constants Cy and Dy such that

    12[(y(T)ˉy(T))2]+ayT0(yˉy)2dtCyQ+Dyem0TQ,

    where y=h,q,f,l, and ah=m0+r+μh, aq=m0+μh+γ, af=m0+μv, al=m0+μv.

    The proof of Claim II is similar to Claim I , we omit it.

    By Claim I and Claim II , we can see that

    12[h(T)ˉh(T)]2+12[q(T)ˉq(T)]2+12[f(T)ˉf(T)]2+12[l(T)ˉl(T)]2+12[ω(0)ˉω(0)]2+12[v(0)ˉv(0)]2+12[j(0)ˉj(0)]2+12[k(0)ˉk(0)]2+(m0+r+μh)T0(hˉh)2dt+(m0+μh+γ)T0(qˉq)2dt+(m0+μv)T0(fˉf)2dt+(m0+μv)T0(lˉl)2dt+(m0+r+μh)T0(ωˉω)2dt+(m0+μh+γ)T0(vˉv)2dt+(m0+μv)T0(jˉj)2dt+(m0+μv)T0(kˉk)2dtC[T0(hˉh)2dt+T0(qˉq)2dt+T0(fˉf)2dt+T0(lˉl)2dt+T0(ωˉω)2dt+T0(vˉv)2dt+T0(jˉj)2dt+T0(kˉk)2dt]+Dem0T[T0(hˉh)2dt+T0(qˉq)2dt+T0(fˉf)2dt+T0(lˉl)2dt+T0(ωˉω)2dt+T0(vˉv)2dt+T0(jˉj)2dt+T0(kˉk)2dt],=(C+Dem0T)Q

    which implies that

    (m0CDem0T)Q0, (4.33)

    where C and D depend on all coefficients and bounds on all solution variables.

    It is easy to see that there exist m0>0 and T>0 sufficiently small such that m0CDem0T0 holds true, that is,

    T<lnm0CDm0.

    For the choice of m0, we have T<lnm0CD. Therefore, the solution to the optimality system (4.17) is unique provided that T sufficiently small. This completes the proof.

    The optimality system (4.17), consisting of the state and the adjoint equations, is solved numerically by using the forward-backward sweep numerical method [37] in the software Matlab. The process begins with an initial estimate for the control pair (u1,u2,u3)=(u10,u20,u30) over the interval [τ,T]. Then, the initial conditions in (4.2) are used to solve the state system forward in time on interval [0,T]. The results obtained for the state variables are plugged into the adjoint equations (4.13). These adjoint equations are then solved backward in time on intervals [Tτ,T] and [0,Tτ], respectively, using the transversality conditions (4.14) and the approximated solution of the state system. Both the state and adjoint values are then used to update the control, and the process is repeated until the current state, adjoint, and controls values converge sufficiently [38].

    Hence, to illustrate the optimal control strategy, different control intervention schemes are compared. The parameter values tabulated in Table 1 and the estimated values of weight constants in the objective functional, are used in the numerical simulations. Based on the actual application, we do not consider single control strategies but focus on evaluating the population-level effectiveness of the following coupled and threefold control combination strategies on the transmission of HLB :

    Strategy I: Combined nutrient solution and infected trees removal strategy (i.e., u10, u20, u3=0).

    Strategy II: Combined nutrient solution and insecticide strategy (i.e., u10, u30, u2=0).

    Strategy III: Combined infected trees removal and insecticide strategy (i.e., u20, u30, u1=0).

    Strategy IV: Combined nutrient solution, infected trees removal and insecticide strategy (i.e., u10, u20, u30).

    The system (4.1) is now simulated to assess the impact of different control strategies on HLB transmission between citrus tree population and psyllid population. For the aforementioned strategies, the optimal solutions for system (4.1) are solved over a time period of 60 months (i.e., T=60 months) and the initial conditions are taken as follows: Sh(0)=1650, Ih(0)=50, Sv(0)=250 and Iv(0)=5. In the simulations, the maximum injecting rate, removing rate and killing rate are taken to be ς1=0.3, ς2=0.6 and ς3=0.8. For the weight factors we choose A1=1000, A2=1, B1=200, B2=1000 and B3=100. It should be pointed out that the weights in the simulations here are only of theoretical sense to illustrate the control strategies proposed in this section. The basic reproductive number in the absence of intervention is given as R0=2.2505. This indicates that if not controlled, HLB will spread rapidly and be epidemic in the grove.

    The results of the optimal control simulations of the HLB model (4.1) are presented in Figures 2, 3, 4 and 5. Firstly, we observe from Figure 2 that the infected citrus trees Ih and infected psyllids Iv increase rapidly without control, while with control, they decrease continuously and tend to be zero eventually. In other words, HLB will die out based on the time-varying optimal control strategy whereas it would break out without control.

    Figure 2.  The number of (a) susceptible trees Sh(t), (b) infected trees Ih(t), (c) susceptible psyllids Sh(t), and (d) infected psyllids Ih(t) with and without control.
    Figure 3.  The number of (a) susceptible trees Sh(t), (b) infected trees Ih(t), (c) susceptible psyllids Sh(t), and (d) infected psyllids Ih(t) under four control strategies, i.e. (i) u1, u2 (u3=0); (ii)u1, u3 (u2=0); (iii) u2, u3 (u1=0); (iv) u1, u2 and u3.
    Figure 4.  Optimal control strategies with three interventions, (a) the efforts of injecting nutrient solution, (b) the efforts of removing the infected trees, (c) the efforts of spraying insecticide.
    Figure 5.  The total cost and the number of infected evolve as the time delay τ increases for a fixed terminal time T = 60 months.

    Secondly, we find that the numbers of susceptible citrus trees Sh, infected citrus trees Ih, susceptible psyllids Sv and infected psyllids Iv under different control strategies are different (see Figure 3). We can see from Figure 3 that the control Strategies III and IV have a very desirable effect upon the population of the citrus trees and the citrus psyllids. To be specific, it is clear that the number of infected individuals reduces significantly in presence of the controls u1, u2 and u3, or u2 and u3. This indicates that nutrient solution has little impact on the prevention of HLB.

    Moreover, after computing total optimal cost and the total infection averted under different strategies (the values are listed in Table 3), we can conclude that the total infection averted is the largest and the total cost is the lowest when implementing Strategy IV. Therefore, for our HLB model, minimizing the total cases of the disease with minimum total cost can be achieved by optimal control strategy IV. We may conclude that Strategy IV is the optimal strategy among the four strategies and it appears to offer a promising measure for HLB control. Additionally, we can see that the total cost of implementing Strategy IV is dramatically less than that of implementing Strategy I or II, and the total infection averted of implementing Strategy IV is more than that of implementing Strategy I or II. This implies application of insecticides and removal of infected trees play an important role in managing HLB transmission.

    Table 3.  The total infection averted and total cost under different strategies.
    Strategies Total infection averted Total cost
    No control 0 1.4066×106
    Strategy I 521.5 6.4369×104
    Strategy II 503.9 1.8934×105
    Strategy III 523.5 1.8843×104
    Strategy IV 523.5 1.8623×104

     | Show Table
    DownLoad: CSV

    The corresponding time-dependent controls u1(t), u2(t) and u3(t) are depicted in Figure 4. We can see that the optimal control variable u1 starts at 0.15, which then increases to 0.96 rapidly in the first 6 months before gradually decreasing to the lower bound 0 at the end of the simulation period. While the optimal control variable u2 starts at the upper bound 1 for over 10 months and slowly decreases to the lower bound 0 at the end of the simulation period. The optimal control variable u3 is similar to u2, it starts at the upper bound 1 for over 20 months and slowly decreases to the lower bound 0 at the end of the simulation period. These results suggest that, in order to economically and effectively control the spread of HLB, nutrient solution control should be only implemented in the start for a short time, while the infected trees removal control and the insecticide control are maintain at high levels for a long time.

    Finally, we present Figure 5 to investigate the effect of delay. Apparently, the longer time delay results in the higher total cost for the stationary terminal time. And we can also see from Figure 5 that there is an increase in the number of infected trees Ih and infected psyllids Iv with the increase of time delay τ. Thus, the longer latent delay leads to HLB control be more complicated, which coincides with the reality. This also implies that ignoring time delay would underestimate the transmission risk of HLB.

    In this paper, we present a new deterministic delayed vector-borne plant model considering disease latency to analyze the spread of HLB, which healthy, infected individuals in the citrus trees and healthy, infected individuals vector populations are taken into consideration. We derive the basic reproductive number R0 and analyze dynamics behavior such as the existence of the equilibria and their stability on the basis of basic reproductive number in two cases τ=0 and τ>0. It shows that the disease-free equilibrium E0 of model (2.1) is globally asymptotically stable if R0<1 and unstable if R0>1, and the endemic equilibrium E is locally asymptotically stable if R0>1 in the case of τ=0; whereas stability changes occur through Hopf bifurcation in our delayed system provided that τ>0.

    Optimal control theory is then applied to investigate the optimal strategy for HLB transmission using three time dependent control variables determined from sensitivity analysis. To the best of our knowledge, no HLB modeling studies have formulated models that incorporate time delay and integrated control. The novel model developed in the current study to explore an optimal integrated strategy for a delayed HLB model considering the disease latency. By using Pontryagin's Maximum Principle, we obtain the exact optimal control formula and prove the uniqueness of optimal control solution. Numerical simulations illustrate the effectiveness of the proposed control problem. The following results are observed from our numerical simulations: (i) effective management of psyllid population will be helpful to curtail the spread of citrus HLB; (ii) the application of three time-dependent controls u1(t), u2(t) and u3(t) obtained from the sensitivity analysis appears to offer a promising measure for HLB control; (iii) threefold control strategy is superior to the coupled control strategies in reducing the spread of HLB; (iv) ignoring time delay would underestimate the transmission risk of HLB.

    As we all know, application of insecticides is the most widely followed option for reducing citrus psyllid population at present. However, some existing literature indicates that the over-reliance on insecticides, their injudicious use and intense selection pressure has resulted in the development of varying levels of resistance in the citrus psyllid population [39,40]. Therefore, there is an urgent need to assess the impact of intensity of insecticides resistance on the transmission dynamics of HLB and explore resistance management strategy that maintains the effective use of all classes of insecticides for citrus psyllids control. We leave this interesting but challenging problem for future investigation.

    Additionally, in [41], the authors illustrate that the seasonal population dynamics of citrus psyllid could be described by trimodal curve. This means the growth rate of psyllid population is strongly impacted by environmental conditions, especially temperature. Therefore, some important features, including the role of temperature-dependent infection rates as well as recruitment of psyllids should be considered in our future work.

    The research has been supported by the Natural Science Foundation of China (11961003, 11901110), The Natural Science Foundation of Jiangxi Province (No.20192ACBL20004), The Science and Technology Project of Education Department of Jiangxi Province (GJJ201406, GJJ1907, GJJ209906), and The Graduate Innovation Project of Jiangxi Province (YC2020-S600).

    All authors declare no conflicts of interest in this paper.



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