Literature DB >> 32308254

A delayed vaccinated epidemic model with nonlinear incidence rate and Lévy jumps.

Kuangang Fan1, Yan Zhang2, Shujing Gao2, Shihua Chen3.   

Abstract

A stochastic susceptible-infectious-recovered epidemic model with nonlinear incidence rate is formulated to discuss the effects of temporary immunity, vaccination, and Le.´vy jumps on the transmission of diseases. We first determine the existence of a unique global positive solution and a positively invariant set for the stochastic system. Sufficient conditions for extinction and persistence in the mean of the disease are then achieved by constructing suitable Lyapunov functions. Based on the analysis, we conclude that noise intensity and the validity period of vaccination greatly influence the transmission dynamics of the system.
© 2019 Elsevier B.V. All rights reserved.

Entities:  

Keywords:  Extinction; Lévy jumps; Nonlinear incidence rate; Stochastic delayed epidemic model; Vaccination

Year:  2019        PMID: 32308254      PMCID: PMC7154516          DOI: 10.1016/j.physa.2019.123379

Source DB:  PubMed          Journal:  Physica A        ISSN: 0378-4371            Impact factor:   3.263


Introduction

Epidemics exert considerable influence on human life. Controlling and eradicating infectious diseases are ongoing problems that have received increasing attention from numerous authors [1], [2], [3], [4], [5], [6]. Various factors, such as vaccination, time delay, impulse and so on, are used to construct mathematical models and seek effective ways to eliminate infectious diseases. Time delay, which has great biologic meaning in epidemic systems, is often used [7], [8], [9], [10]. Many scholars have also paid close attention to the effects of the temporary disease immunity of epidemic models, i.e., a fleeting immunity to a disease after recovery before becoming susceptible again. The phenomenon is common during the transmission of many epidemic diseases, such as influenza, Chlamydia trachomatis, Salmonella and so on. Thus, in current paper, we introduce temporal delays to make epidemic models more realistic and interesting. Epidemic models are inevitably subject to environmental noise. Most epidemic models are driven by white noise, and many results have been achieved in this area [11], [12], [13], [14], [15], [16], [17], [18], [19]. However, under severe environmental perturbations, such as avian influenza, severe acute respiratory syndrome, volcanic eruptions, earthquakes, and hurricanes, the continuity of solutions may be broken; accordingly, a jump process should be introduced to prevent and control diseases [20], [21], [22], [23]. In the present work, we consider the effects of vaccination and temporary immunity on a stochastic susceptible–infectious–recovered (SIR) epidemic model driven by Lévy noise. A generalized nonlinear incidence rate is also introduced. Based on the above factors, we formulate the delayed vaccinated SIR epidemic model as follows: where , , and are the numbers of susceptible, infectious, and recovered populations, respectively. represents the constant recruitment of susceptible individuals, is the natural death rate of populations, is the transmission rate, represents the recovery rate, denotes the proportional coefficient of the vaccinated for the susceptible, represents the validity period of the vaccination and is the length of the immunity period. All parameters are assumed to be positive constants. Herein, is the intensity of white noise and ; and is the standard Brownian motions, which are defined on a complete probability space with filtration satisfying the usual conditions [21]. is a Poisson counting measure with compensator and characteristic measure on a measurable subset of which satisfies ; is assumed to be a lévy measure, such that ; is bounded and continuous with respect to and is -measurable, where is a -algebra with respect to the set , is a sub -algebra of , and is a -algebra of subsets of a given set  [22]. In this paper, and are assumed to be independent of each other. As the first two equations do not depend on the last equation in system (1.1), therefore, we only consider the equations as follows: The initial conditions of model (1.2) are where is the space of continuous functions mapping the interval into , herein, , . According to the phenomena observed in nature, such as bee colonies, we assume that the self-regulating competitions within the same species are strictly positive, that is, Assumption (H1) is a bounded function and , . We also establish the following assumptions on functions and : Assumption (H2) is a continuously differentiable function and monotonically increasing on , . A constant exists, such that , and . Assumption (H3) is twice continuously differentiable, and is monotone decreasing on , , and . The aim of this paper is to prove the existence and uniqueness of a global positive solution. The extinction and persistence in the mean of the system are also discussed.

Preliminaries

In this section, we list some notations, definitions and lemmas. First, we denote where is a continuous and bounded function defined on . Then, we give the It’s formula for general stochastic differential equations. Define the -dimensional stochastic equation [24]: with initial value . Here, is a -dimensional vector function, is a matrix function and is a dimensional standard Brownian motion defined on the probability space . Define the differential operator associated with Eq. (2.1) If function , then we have Thus, the It’s formula is listed as follows

[24]

Let satisfy Eq. (2.1) and function . Then here, .

[25]

Suppose that , here . and there exists a positive constant such that , then If positive constants , and exist such that for all , where is a constant, , then, If positive constants , and exist such that for all , then, .

Existence and uniqueness of the global solution

Denote and then we discuss the existence and uniqueness of the global positive solution and the positive invariant of system (1.2) with positive initial value (1.3). If Assumption (H1) hold, then for any initial value , a unique solution of system (1.2) exists on and the solution will remain in with probability one. According to the local Lipschitz condition of system (1.2), we obtain that for any initial value , a unique local solution exists on , herein, represents the explosion time. To prove that the solution is global, it is required to obtain that a.s. Then, we suppose that is sufficiently large such that and lie within the interval . For each integer , we define the stopping time . Then, increases as . Denote , thus . In the following, we need to show that . If not, there are constants and satisfying . Thus, an integer exists such that , for all . Construct a -function by where is a constant that will be given later. By virtue of ’s formula, we derive Here, is defined as follows where , , and we choose . On the other hand, we achieve that Thus, Then applying Taylor formula to function here and Assumption (H1) to , we have that Here is an arbitrary number. Similarly, we can obtain that Then Therefore, we achieve that Taking integral on the above inequality from to , then where . Consequently, Let , then . For each , , or equals either or , and Thus, where is the indicator function of . Letting , we obtain the contradiction. The proof is completed. Next, we prove that is a positively invariant set of system (1.2). The region is almost surely positive invariant of system (1.2) . Suppose , and be sufficiently large such that and . For each integer , the stopping times are defined as follows We need to show that for all . Notice that , then we have to prove . Define the function then here, Then Thus, where Taking integral and expectation on both sides of (3.7) and by virtue of Fubini Theorem, then we derive Applying Gronwall Lemma, we obtain that for all . Thus, In consideration of and some component of being less than or equal to , we achieve that By (3.8), (3.9), we obtain that for all . Therefore, The proof is completed.

The extinction of diseases

In this section, to discuss the extinction of the disease, we define and for the sake of simplicity, we denote , then the following theorem is obtained. Suppose be any solution of system (1.2) with an initial value (1.3) . Thus (1) If , then (2) If and , then where . Applying It’s formula, we derive that Then Here, and . on the other hand, we have then, Therefore, and here, , thus . According to (4.5), we obtain that where In addition, and Then, we have that and Thus, By virtue of the condition (2) and (4.6), we achieve that Moreover, by (4.6), we have that According to the condition (1) and (4.8), we obtain that That is . Moreover, we have that The conclusion is proven. From Theorem 4.1, we show that if condition (i) , or (ii) and hold, then for an arbitrary solution of system (1.2), we have , which implies that the disease is extinct.

Persistence in the mean of system

Now we are in the position to discuss the persistence in the mean of the disease and before that some notations are presented in the following. For the convenience, we denote Suppose that Assumption (H1) hold and then for the solution of model (1.2) , (1) If , we have (2) If and , we have Since , then a constant exists satisfying for all . By virtue of (4.6), we have that Then here, . Considering , then for an arbitrary , there exists a and a set such that and for all , . Let , then according to Lemma 2.2 and Theorem 3 in Ref. [22], we achieve that On the other hand, by (4.2), (4.5), we obtain that As , then we derive that . Thus, By virtue of the conclusion and the arbitrariness of , we obtain that In addition, by virtue of (4.5), (5.6), we have that In the following , we prove By assumptions (H2) and (H3), a constant exists satisfying for all . Using the first equation of model (1.2), we achieve that Therefore, by Theorem 4.1 and applying the arbitrariness of , we have The desired result is obtained. From Theorem 5.1, we obtain that if , and choose , then the solution of system (1.2) with an initial condition (1.3) is persistent in the mean. Moreover, denote , we can also obtain the condition for the permanence in the mean of the system, that is, and

Numerical simulations

In this section, we will perform some numerical simulations to illustrate our theoretical results by Euler numerical approximation [26]. (1) Choose the parameter values in model (1.2) as follows: and the only difference between conditions of Fig. 1, Fig. 2 is the different values .
Fig. 1

The disease I of system (1.2) goes to extinction with probability one. The red lines, the green lines and the blue lines are solutions of system (1.2), the corresponding deterministic system and the system with white noise, respectively.

Fig. 2

The disease I of system (1.2) is persistent with probability one. The red lines, the green lines and the blue lines are solutions of system (1.2), the corresponding deterministic system and the system with white noise, respectively.

The disease I of system (1.2) goes to extinction with probability one. The red lines, the green lines and the blue lines are solutions of system (1.2), the corresponding deterministic system and the system with white noise, respectively. The disease I of system (1.2) is persistent with probability one. The red lines, the green lines and the blue lines are solutions of system (1.2), the corresponding deterministic system and the system with white noise, respectively. In Fig. 1, the intensities of the noises are and , then we have that and the condition (1) of Theorem 4.1 is satisfied. Thus, the disease goes to extinction with probability one and Fig. 1 confirms it. Moreover, by Fig. 1, we achieve that the disease is extinct whereas the corresponding deterministic system is persistent because of the effect of the jump noise. In Fig. 2, the intensities of the noises are and , then we obtain that and the condition (1) of Theorem 5.1 holds. Therefore, the disease is persistent with probability one. (2) Let and the other parameters are the same as those in Fig. 1. Considering different values of and , then we can observe the effects of the validity period of the vaccination to system (1.2) (See Fig. 3).
Fig. 3

The effects of the validity period to system (1.2).

The effects of the validity period to system (1.2). From Fig. 1, Fig. 2, Fig. 3, we achieve that the intensity of Lévy noise and the validity period of the vaccination can greatly influence the extinction and persistence of the disease .

Conclusion

A stochastic delay epidemic model is proposed with vaccination and generalized nonlinear incidence rate. The effects of Lévy jumps are considered in this model. The existence of a unique global solution is proven. Sufficient conditions that guarantee diseases to be extinct and persistent in the mean are given. From the analysis and discussion, we derive that noise intensity and the validity period of vaccination greatly influence the extinction and persistence of diseases. Finally, some interesting issues merit further investigations. In this paper, we obtain sufficient conditions for the persistence and extinction of the model. However, whether the threshold value could be derived is an interesting issue. In addition, if we also consider the effects of non-autonomous environment to the proposal of epidemic model, how will the properties change? We will investigate these questions in our future work.

Declaration of Competing Interest

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