#### Abstract

In this paper, by introducing environmental perturbation, we extend an epidemic model with graded cure, relapse, and nonlinear incidence rate from a deterministic framework to a stochastic differential one. The existence and uniqueness of positive solution for the stochastic system is verified. Using the Lyapunov function method, we estimate the distance between stochastic solutions and the corresponding deterministic system in the time mean sense. Under some acceptable conditions, the solution of the stochastic system oscillates in the vicinity of the disease-free equilibrium if the basic reproductive number , while the random solution oscillates near the endemic equilibrium, and the system has a unique stationary distribution if . Moreover, numerical simulation is conducted to support our theoretical results.

#### 1. Introduction

Mathematical models can improve our understanding of the dynamics of infectious diseases, predict the transmission trend, and help us formulate preventive measures. The classical and epidemic models established by Kermack and McKendrick are one of the most important models in epidemiology [1, 2]. From then on, a large number of researchers have proposed and investigated more accurate epidemic models, taking into account different forms of incidence rate, intervention strategies, random perturbation, and other factors. In particular, the human body has certain immune mechanisms to keep itself healthy, and individuals recovered from some diseases may relapse and become reinfected . Therefore, it is natural to consider immune effects in mathematical models. Recently, to explore infectious diseases in which infected individuals may be permanently rehabilitated or reinfected, Lahrouz et al.  proposed a nonlinear epidemic model with relapse and graded cure as follows:where , , and denote the numbers of the population that are susceptible, infective, and recovered with temporary immunity, respectively. The parameter is the growth rate of ; denotes the death rates of , , and , respectively; is the recovery rate of ; , , and denote the relapse rate, the temporary immunity, and cure rate, respectively; is the transmission rate from to . All the parameters are assumed to be positive, and it is biologically meaningful to suppose that . The nonlinear incidence rate in model (1) reflects the heterogeneous mixing of susceptible and infective population, and the force of infection is a function of on such that

Lahrouz et al.  have studied the global dynamics of system (1). The basic reproduction number is computed asand the unique disease-free equilibrium is globally asymptotically stable if . Under some additional conditions, system (1) has a unique endemic equilibrium and it is globally asymptotically stable if .

A large amount of research studies have found that the spread of diseases is naturally subject to random environmental perturbation, such as unpredictable human exposure and meteorological factors [8, 9]. Hence, an increasing number of stochastic epidemic models including environmental noise have been developed . In the present paper, motivated by the approach in [14, 15], we introduce system (1) environmental noise which is directly proportional to , , and and establish the following stochastic system:

Throughout the paper, we let be a complete probability space with a filtration satisfying the usual conditions (i.e., it is increasing and right continuous while contains all -null sets), denotes a scalar Brownian motion defined on the complete probability space , and .

The rest of the paper is organized as follows. In Section 2, we prove the existence and uniqueness of the positive solution for system (4), and some long time behavior of the solution is discussed. In Section 3, we analyze the asymptotic behavior of system (4) near the disease-free equilibrium and estimate the distance between stochastic solutions and the corresponding deterministic system in the time mean sense. In Section 4, asymptotic behavior near endemic equilibrium is analyzed, and we also obtain sufficient conditions for the existence of stationary distribution and persistence of diseases. In Section 5, numerical simulation is displayed to support our theoretical results. A brief conclusion is given in the last section.

#### 2. Existence and Uniqueness of the Positive Solution

In this section, we present two main results. The first theorem guarantees the existence and uniqueness of the positive solution for system (4), and the second one shows some long time behavior of the solution.

Theorem 1. For any initial value , there exists a unique positive solution for system (4) on and the solution will remain in with probability one.

Proof. Since the coefficients of system (4) are locally Lipschitz continuous, then for any initial value there is a unique local solution on , where is the explosion time. Moreover, the unique local solution to model (4) is positive by Itô’s formula . Therefore, it suffices to verify that the solution is global, i.e., a.s. Let be sufficiently large such that , and lie within the interval . For each integer , define the stopping times:Set ( represents the empty set). Note that is increasing as . Let , then a.s. Now, we state that a.s. If this statement is violated, then there exists a constant and such that . As a consequence, there exists an integer such thatDefine a nonnegative -function aswhere is a positive constant determined later, and the nonnegativity can be obtained from .
Let and be arbitrary. Applying Itô’s formula to , we obtain thatwhereHere, we choose such that . Then, substituting the inequality into (8) yields thatFurthermore,where . Taking the expectation of the above inequality yieldsSet for , then due to (6). Note that, for every , at least one of equals to either or . Hence,Following from (12), we obtainwhere is the indicator function of . Taking , we have , which is a contradiction. The conclusion is confirmed.

Theorem 2. For any initial value , the solution of system (4) has the following properties:The proof is standard, and we omit it here.

#### 3. Asymptotic Behavior around the Disease-Free Equilibrium

For the deterministic system (1), the unique disease-free equilibrium is globally asymptotically stable if the reproduction number . The following theorem shows the asymptotic behavior of the stochastic system (4) near .

Theorem 3. Let be the solution of system (4) with any initial value . If , and , thenwhere .

Proof. Define functions as follows:Making use of Itô’s formula, we obtainwhereAs , we haveSimilarly,In inequalities (19)–(22), we have used the inequality for any , and the young inequality .
Define a nonnegative function as follows:Together with (19)–(22), we obtainIntegrating both sides of (24) and taking expectation, we obtainHence,The above theorem shows that the solution of system (4) oscillates near the disease-free equilibrium in the time mean sense if , and the magnitude of the oscillation is proportional to the intensity of noise. From the perspective of biology, the disease will be controlled in a small range if the intensity of noise is sufficiently small.

#### 4. Stationary Distribution and Asymptotic Behavior around the Endemic Equilibrium

In this section, we turn to the case when the reproduction number and discuss sufficient conditions for the persistence of disease. We first recall some general results. Consider -dimension stochastic equation:where is a homogeneous Markov process in -dimension Euclidean space . The diffusion matrix is defined as follows:

Lemma 1. (see ). The Markov process X(t), the solution of system (27), has a unique ergodic stationary distribution , if there exists a bounded domain with regular boundary and(i)There exists a positive number such that , , .(ii)There exists a nonnegative function such that is twice continuously differentiable and that for some , , for any . Then,for all , where be a function integrable with respect to the measure .
For the deterministic system (1), there exists at least one positive equilibrium if . Moreover, assume the conditionholds; then, the equilibrium is unique and globally stable according to Theorem 5.1 in .

Theorem 4. Let , and assume conditions (2) and (30) hold. If , then for any initial value , system (4) has a unique stationary distribution and the ergodicity hold. Especially, we haveHere, , and .

Proof. In order to prove the existence of a unique ergodic stationary distribution, it suffices to verify conditions (i) and (ii) in Lemma 1. To begin with, it is easy to see that satisfiesDefine nonnegative functions as follows:By a standard calculation, we obtainThen, define a nonnegative function :According to (34)–(36), it impliesDenote an ellipsoid , then the ellipsoid lies entirely in if . Take to be any neighborhood of with , then there exists some such that for any . That is, condition (ii) holds.
The diffusion matrix of system (4) is given byChoose , we haveThen, condition in Lemma 1 is satisfied. Therefore, according to Lemma 1, the stochastic system (4) has a unique stationary distribution and it is ergodic. Moreover, the dynamical behavior around the endemic equilibrium satisfiesThe proof is completed.
Theorem 4 shows that, under certain conditions, the solution of system (4) will oscillate around the endemic equilibrium for the long time. Furthermore, the following theorem indicates that the disease will be almost surely persistent in the time mean sense.

Theorem 5. Suppose the conditions in Theorem 4 hold; then, the solution of system (4) has the property that

Proof. According to the proof process of Theorem 4, we haveIntegrating the above inequality from 0 to , we obtainwhereFrom the strong law of large numbers for local martingales, we have Thus, , which implies thatFurthermore, we haveDue to , it deducesSubstituting (48) into (47), we obtainTherefore, the disease is persistent in the sense of time mean. The proof is completed.

#### 5. Numerical Simulations

In this section, we choose the saturation incidence function as in . Using Milstein’s higher order method , we obtain the following discrete equations with respect to system (4):

Here, the time increment , and , , and , are independent Gaussian random variables , and , , are intensities of white noise. Choose the initial value , and the value of parameters as . The selection of these parameters satisfies the condition of Theorem 3, and numerical simulation is displayed in Figure 1. Moreover, we can see that when the noise intensity decreases, and the vibration of the solution for system (4) also decreases.

Similarly, take the value of parameters as