Loading [MathJax]/jax/output/SVG/jax.js
Research article

A new class of Appell-type Changhee-Euler polynomials and related properties

  • Received: 07 July 2021 Accepted: 06 September 2021 Published: 24 September 2021
  • MSC : 11B68, 33B10, 33E20

  • A remarkably large number of polynomials and their extensions have been presented and studied. In the present paper, we introduce the new type of generating function of Appell-type Changhee-Euler polynomials by combining the Appell-type Changhee polynomials and Euler polynomials and the numbers corresponding to these polynomials are also investigated. Certain relations and identities involving these polynomials are established. Further, the differential equations arising from the generating function of the Appell-type Changhee-Euler polynomials are derived. Also, the graphical representations of the zeros of these polynomials are explored for different values of indices.

    Citation: Tabinda Nahid, Mohd Saif, Serkan Araci. A new class of Appell-type Changhee-Euler polynomials and related properties[J]. AIMS Mathematics, 2021, 6(12): 13566-13579. doi: 10.3934/math.2021788

    Related Papers:

    [1] Lu-Chuan Ceng, Li-Jun Zhu, Tzu-Chien Yin . Modified subgradient extragradient algorithms for systems of generalized equilibria with constraints. AIMS Mathematics, 2023, 8(2): 2961-2994. doi: 10.3934/math.2023154
    [2] Pongsakorn Yotkaew, Nopparat Wairojjana, Nuttapol Pakkaranang . Accelerated non-monotonic explicit proximal-type method for solving equilibrium programming with convex constraints and its applications. AIMS Mathematics, 2021, 6(10): 10707-10727. doi: 10.3934/math.2021622
    [3] Fei Ma, Jun Yang, Min Yin . A strong convergence theorem for solving pseudo-monotone variational inequalities and fixed point problems using subgradient extragradient method in Banach spaces. AIMS Mathematics, 2022, 7(4): 5015-5028. doi: 10.3934/math.2022279
    [4] Habib ur Rehman, Wiyada Kumam, Poom Kumam, Meshal Shutaywi . A new weak convergence non-monotonic self-adaptive iterative scheme for solving equilibrium problems. AIMS Mathematics, 2021, 6(6): 5612-5638. doi: 10.3934/math.2021332
    [5] Yali Zhao, Qixin Dong, Xiaoqing Huang . A self-adaptive viscosity-type inertial algorithm for common solutions of generalized split variational inclusion and paramonotone equilibrium problem. AIMS Mathematics, 2025, 10(2): 4504-4523. doi: 10.3934/math.2025208
    [6] Rose Maluleka, Godwin Chidi Ugwunnadi, Maggie Aphane . Inertial subgradient extragradient with projection method for solving variational inequality and fixed point problems. AIMS Mathematics, 2023, 8(12): 30102-30119. doi: 10.3934/math.20231539
    [7] Bancha Panyanak, Chainarong Khunpanuk, Nattawut Pholasa, Nuttapol Pakkaranang . A novel class of forward-backward explicit iterative algorithms using inertial techniques to solve variational inequality problems with quasi-monotone operators. AIMS Mathematics, 2023, 8(4): 9692-9715. doi: 10.3934/math.2023489
    [8] Lu-Chuan Ceng, Shih-Hsin Chen, Yeong-Cheng Liou, Tzu-Chien Yin . Modified inertial subgradient extragradient algorithms for generalized equilibria systems with constraints of variational inequalities and fixed points. AIMS Mathematics, 2024, 9(6): 13819-13842. doi: 10.3934/math.2024672
    [9] Francis Akutsah, Akindele Adebayo Mebawondu, Austine Efut Ofem, Reny George, Hossam A. Nabwey, Ojen Kumar Narain . Modified mildly inertial subgradient extragradient method for solving pseudomonotone equilibrium problems and nonexpansive fixed point problems. AIMS Mathematics, 2024, 9(7): 17276-17290. doi: 10.3934/math.2024839
    [10] Austine Efut Ofem, Jacob Ashiwere Abuchu, Godwin Chidi Ugwunnadi, Hossam A. Nabwey, Abubakar Adamu, Ojen Kumar Narain . Double inertial steps extragadient-type methods for solving optimal control and image restoration problems. AIMS Mathematics, 2024, 9(5): 12870-12905. doi: 10.3934/math.2024629
  • A remarkably large number of polynomials and their extensions have been presented and studied. In the present paper, we introduce the new type of generating function of Appell-type Changhee-Euler polynomials by combining the Appell-type Changhee polynomials and Euler polynomials and the numbers corresponding to these polynomials are also investigated. Certain relations and identities involving these polynomials are established. Further, the differential equations arising from the generating function of the Appell-type Changhee-Euler polynomials are derived. Also, the graphical representations of the zeros of these polynomials are explored for different values of indices.



    Leptospirosis is an acute systemic infectious disease caused by various pathogenic leptospira, which belongs to natural foci disease. It is epidemic almost all over the world, especially severe in Southeast Asia. Most provinces, cities, and autonomous regions in China have the existence and epidemic of this disease. Rodents and pigs are the two major sources of infection, while other livestock such as cattle, pigs, and pets like cats, dogs, and mice may also transmit leptospirosis. Typically, pathogenic leptospira can survive longer in a warm and humid environment. People may contract the disease through ingestion of contaminated food or water, or when the bacteria enter the body through scratches on the skin or mucous membranes [1].

    The application of mathematical models in leptospirosis research has also become increasingly widespread. Through numerical simulations and data analysis, we can delve deeper into the transmission mechanisms and dynamic characteristics of the disease, providing more precise and effective means for disease prevention and control. Regarding the research on mathematical models of leptospirosis, please refer to the literature [2,3,4,5,6]. These models analyze the factors that influence the transmission dynamics of leptospirosis, pointing out that disease transmission is not only related to the interaction between rodents and humans [4], but also to their contact with free bacteria in the environment [6]. They also demonstrate that adopting appropriate intervention mechanisms, such as reducing the transmission rate, increasing the recovery rate, reducing rodent populations, and reducing bacterial contamination in water sources, can greatly assist in reducing the spread of the disease in the population.

    In the real world, infectious disease models are inevitably affected by environmental noise, and deterministic models alone cannot accurately reflect the dynamic behavior of the system when describing disease transmission processes. In recent years, most scholars have explored stochastic infectious disease models that consider environmental perturbations [7,8,9,10,11,12]. The research results indicate that random perturbations have a certain impact on the spread of diseases.

    Therefore, it is highly necessary to further establish and study leptospirosis models that consider vector-environment interactions and random disturbances.

    To establish the model, we make the following assumptions.

    (ⅰ) Susceptible individuals who come into contact with infected vectors or free bacteria in the environment can become infected individuals, and susceptible vectors that come into contact with infected individuals or free bacteria in the environment can also become infected vectors.

    (ⅱ) Infected individuals and vectors both release free bacteria into the environment.

    (ⅲ) The host population Sh(t),Ih(t),Sh(t), vector population Sv(t),Iv(t), and the concentration of bacteria in the environment are all influenced by Gaussian white noise.

    (ⅳ) The recruitment rate Λ and the birth rate Π of the vectors are constants. Every parameter within the system is a nonnegative real number.

    Base on the above assumptions, we establish and study a stochastic model of leptospirosis with host-vector-environment interactions:

    {dSh(t)=[ΛμhShβ1ShIvNhβ3ShBK+B+λhRh]dt+σ1ShdB1(t),dIh(t)=[β1ShIvNh+β3ShBK+BμhIhδhIhγhIh]dt+σ2IhdB2(t),dRh(t)=[γhIhλhRhμhRh]dt+σ3RhdB3(t),dSv(t)=[Πβ2IhSvNhβ4SvBK+BμvSv]dt+σ4SvdB4(t),dIv(t)=[β2IhSvNh+β4SvBK+BμvIv]dt+σ5IvdB5(t),dB(t)=[α1Ih+α2IvkB]dt+σ6BdB6(t), (1.1)

    where the host population, which represents the human population, is divided into three categories at time t: susceptible individuals Sh(t), infected individuals Ih(t), and recovered individuals Rh(t). The vector population is divided into susceptible vectors Sv(t) and infected vectors Iv(t) at time t. Additionally, B(t) represents the free-floating bacterial population in the environment. The meanings of the parameters are as follows. β1 and β2 represent the infection rates of diseased vectors transmitting the disease to humans and of infected humans transmitting the disease to vectors, respectively. β3 and β4 represent the rates at which susceptible humans and susceptible vectors become infected through contact with bacteria in the environment. μh and μv are natural mortality rate for the human population and the vector population, and γh represents the disease-induced mortality rate among humans. δh represents the recovery rate for infected humans, while λh represents the rate at which recovered humans revert back to the susceptible state. α1 and α2 represent the rates at which infected humans and infected vectors release bacteria into the environment, respectively. K serves as a half-saturation infection parameter, and k is the decay rate of bacteria in the environment. Bi(t)(i=1,2,3,4,5,6) are standard Brownian motions. Parameters σi(i=1,2,,6) are the intensities of noise, representing variability and stochastic effects: σ1 represents the variability in the susceptible individuals Sh(t), which arise from fluctuating contact rates or changes in population behavior that affect exposure to the virus environment and infected vectors; σ2 reflects the random fluctuations in the number of the infected population Ih(t) due to variations in the disease's infectiousness, or response to treatment; σ3 represents stochastic factors affecting the recovered population Rh(t), such as loss of immunity or the impact of interventions; σ4 represents the variability in the susceptible vectors Sv(t), which arise from fluctuating contact rates or changes in population behavior that affect exposure to the Leptospira virus environment and infected individuals; σ5 reflects the random fluctuations in the number of the infected vectors Iv(t) due to variations in the disease¡¯s infectiousness; σ6 represents the random variation intensity of Leptospira virus B(t) released into the environment by infected humans or disease vectors.

    We assume the initial conditions are

    Sh(0)0,Ih(0)0,Rh(0)0,Sv(0)0,Iv(0)0,B(0)0. (1.2)

    The aim of this paper is to build a stochastic model of leptospirosis that incorporates both vector-borne and environmental transmission to more comprehensively describe the disease's transmission characteristics. Furthermore, by combining this model with actual reported data on leptospirosis in China in recent years, we aim to estimate important parameters of the model using statistical methods and predict the future trends of leptospirosis in China.

    To demonstrate that our proposed model is meaningful, we prove that there exists a unique global positive solution of the system (1.1).

    Theorem 2.1. For any initial value (Sh(0),Ih(0),Rh(0),Sv(0),Iv(0),B(0))R6+, the system (1.1) has a unique positive solution (Sh(t),Ih(t),Rh(t),Sv(t),Iv(t),B(t)), and the solution will remain in R6+ with probability 1, i.e., (Sh(t),Ih(t),Rh(t),Sv(t),Iv(t),B(t))R6+ for all t>0 almost surly (a.s.).

    Proof. Obviously, the system (1.1) has locally Lipschitz continuous coefficients, for any initial value (Sh(0),Ih(0),Rh(0),Sv(0),Iv(0),B(0))R6+, and the system (1.1) exists a unique maximal local solution (Sh(t),Ih(t),Rh(t),Sv(t),Iv(t),B(t)), t[0,τe), where τe is the explosion time. To verify that this solution of the system (1.1) is global, we just have to prove that τe= a.s. For this, assume k01 is large enough such that (Sh(0),Ih(0),Rh(0),Sv(0),Iv(0),B(0)) all fall within the interval [1/k0,k0]. For each integer kk0, define the stopping time as:

    τk=inf{t[0,τe):Sh(t)(1k,korIh(t)(1k,korRh(t)(1k,k)orSh(t)(1k,korIv(t)(1k,k)orB(t)(1k,k)},

    where inf= ( denotes the empty set). Clearly, when k, τk are increasing. Let τ=limkτk, then ττe a.s. If τ= a.s. holds, then τe= a.s., which means that (Sh(t),Ih(t),Rh(t),Sv(t),Iv(t),B(t))R6+ a.s. for t0. Therefore, it suffices to prove that τ= a.s.

    Next, we assume that there exist constants T>0 and ε(0,1), such that P{τT}>ε, then, there exists an integer k1k0, such that for any kk1,

    P{τkT}ε. (2.1)

    Define the function Q:R6+R+ as follows:

    Q(Sh,Ih,Rh,Sv,Iv,B)=(Sha1a1lnSha1)+(Ih1lnIh)+(Rh1lnRh)+(Svb1b1lnSvb1)+(Iv1lnIv)+ln(1+1B),

    where a1,b1 are positive constants to be determined later. Obviously, the function u1lnu is non-negative for all u>0.

    Applying Itô's formula, we obtain

    dQ=LQdt+σ1(Sha1)dB1(t)+σ2(Ih1)dB2(t)+σ3(Rh1)dB3(t)+σ4(Svb1)dB4(t)+σ5(Iv1)dB5(t)σ61+BdB6(t),

    where

    LQ=Λμh(Sh+Ih+Rh)δhIh+Πμv(Sv+Iv)α1IhB(1+B)α2IvB(1+B)+k1+Ba1ΛSh+a1μh+a1β1IvNh+a1β3BK+Ba1λhRhShβ1ShIvNhIhβ3ShB(K+B)Ih+μh+δh+γhγhIhRh+λh+μhb1ΠSv+b1β2IhNh+b1β4BK+B+b1μvβ2SvIhNhIvβ4SvB(K+B)Iv+μv+12a1σ21+12σ22+12σ23+12b1σ24+12σ25+121+2B(1+B)2σ26Λ+Π+k+a1μh+(a1β1M1μv)Iv+a1β3+μh+δh+γh+λh+μh+(b1β2M1μh)Ih+b1β4+b1μv+μv+12a1σ21+12σ22+12σ23+12b1σ24+12σ25+12σ26.

    Choose a1=μvM1β1,b1=μhM1β2, such that a1β1M1μv=0,b1β2M1μh=0, and

    LQΛ+Π+k+a1μh+a1β3+μh+δh+γh+λh+μh+b1β4+b1μv+μv+12a1σ21+12σ22+12σ23+12b1σ24+12σ25+12σ26:=K,

    where K>0 is a constant. The remainder of the proof follows the similar approach given in [13].

    Now, the sufficient conditions for the elimination of Ih,Iv are presented. Denote f=1tt0f(s)ds, and the parameter as follows:

    Rm=(β1+β2+β4)μhΠ+β3μvΛμhμv(Λ+Π)+(δh+γh)μvΛ.

    To facilitate the proof of the theorem, we first give a related lemma.

    Lemma 2.1. [14,15,16] For any initial value (Sh(0),Ih(0),Rh(0),Sv(0),Iv(0),B(0))R6+, the solution (Sh(t),Ih(t),Rh(t),Sv(t),Iv(t),B(t))R6+ of model (1.1) possesses the following properties:

    limtt0Sh(s)dB1(s)t=0, limtt0Ih(s)dB2(s)t=0, limtt0Rh(s)dB3(s)t=0, 
    limtt0Sv(s)dB4(s)t=0, limtt0Iv(s)dB5(s)t=0, limtt0B(s)dB6(s)t=0 a.s.

    Proof of Lemma 2.1 can be similarly obtained by following the proof of Lemma 2.2 in reference [14]. The details are omitted here.

    Theorem 2.2. Assume (Sh(t),Ih(t),Rh(t),Sv(t),Iv(t),B(t))R6+ is the solution of model (1.1) that satisfies the initial condition (Sh(0),Ih(0),Rh(0),Sv(0),Iv(0),B(0))R6+. If Rm<1, then (Ih(t),Iv(t),B(t)) converges to (0,0,0) exponentially with probability one (a.s.), indicating the elimination of the disease, and furthermore,

    limtSh(t)=Λμh, limtSv(t)=Πμv, limtRh(t)=0 a.s.

    Proof. Let P(t)=Ih(t)+Iv(t). Applying Itô's formula, we have

    dP(t)=[β1ShNhIv+β3ShBK+BμhIhδhIhγhIh+β2IhNhSv+β4SvBK+BμvIv]dt+σ2IhdB2(t)++σ5IvdB5(t). (2.2)

    Integrating both sides of (2.2) from 0 to t and dividing by t, we obtain

    P(t)t=P(0)t+β1ShNhIv+β3ShBK+B(μh+δh+γh)Ih+β2IhNhSv+β4SvBK+BμvIv+1tt0σ2Ih(s)dB2(s)+1tt0σ5Iv(s)dB5(s)P(0)t+β1Iv+β3Sh(μh+δh+γh)Ih+β2Sv+β4SvμvIv+1tt0σ2Ih(s)dB2(s)+1tt0σ5Iv(s)dB5(s). (2.3)

    Notice

    d(Sh(t)+Ih(t)+Rh(t))[Λμ(Sh+Ih+Rh)]dt+σ1Sh(t)dB1(t)+σ2Ih(t)dB2(t)+σ3Rh(t)dB3(t) (2.4)

    and

    d(Sv(t)+Iv(t))=[Πμv(Sv+Iv)]dt+σ4Sv(t)dB4(t)+σ5Iv(t)dB5(t). (2.5)

    Integrating both sides of (2.4) and (2.5) from 0 to t and dividing by t, then, taking the upper limit, we obtain

    lim suptSh(t)+Ih(t)+Rh(t)Λμh a.s.
    lim suptSv(t)+Iv(t)=Πμv a.s.

    Thus

    lim suptSh(t)Λμh, lim suptIh(t)Λμh, lim suptRh(t)Λμh a.s.
    lim suptSv(t)Πμv, lim suptIv(t)Πμv a.s.

    Taking the upper limit of both sides of (2.3), and according to Lemma 2.1, we can obtain the desired result

    lim suptP(t)tβ1Πμv+β3Λμh(μh+δh+γh)Λμh+β2Πμv+β4ΠμvμvΠμv=μh(Λ+Π)+(δh+γh)Λμh(Rm1)<0.

    Then

    limtP(t)=0.

    Hence

    limtIh(t)=0, limtIv(t)=0.

    For the sixth equation in (1.1), by integrating both sides from 0 to t, dividing by t, and then taking the upper limit, we can derive that limtB(t)=0.

    Similarly, applying the same method to the third equation in (1.1), we can obtain limtRh(t)=0.

    Since

    d(Sh(t)+Ih(t))=[ΛμhShμhIhδhIhγhIh+λhRh]dt+σ1Sh(t)dB1(t)+σ2Ih(t)dB2(t),

    based on the conclusions obtained above, we can derive that limtSh(t)=Λμh. Similarly, we can obtain that limtSv(t)=Πμv.

    To better analyze the impact of different parameters on the spread of infectious diseases on the surface, we will proceed with a further parameter sensitivity analysis. We conduct 1000 samplings of the parameters using the Latin Hypercube Sampling (LHS) method [17]. By calculating the Partial Rank Correlation Coefficient (PRCC), we will be able to screen out the parameters that have a significant impact on the population size. This will help us identify more accurate measures to control the epidemic.

    Observing Figure 1, it is evident that the parameters with significant impacts on disease transmission are β3,δh,γh,μv. Here, β3 is positively correlated with Rm, while δh,γh,μv are negatively correlated with Rm. In other words, the smaller the contact rate of humans with free bacteria in the environment, the higher the human mortality rate due to the disease and the natural mortality rate of the vector population; and the faster the recovery rate from the disease, the smaller the basic reproduction number will be, making it easier to eliminate the disease. In fact, as the contact rate of humans with free bacteria in the environment declines, so does the likelihood of contracting the virus. Similarly, when the mortality rate stemming from the illness is high, infected individuals may perish during the infection period, thereby diminishing their capacity to spread the disease to others, resulting in a lower average transmission rate per infected individual. Furthermore, a high natural mortality rate among vectors lessens their chances of transmitting the disease to humans and curtails the release of virus particles into the environment. Lastly, an increase in the recovery rate of infected individuals reduces their chances of transmitting the disease to vectors. All these scenarios contribute significantly to a decrease in the Rm value.

    Figure 1.  The correlation PRCC index of each parameter on Rm.

    Next, we perform numerical simulations on the system (1.1) by using the high-order Milstein method mentioned in [18,19], which is based on the concept of Itô's formula and stochastic Taylor expansion. The Milstein method improves the accuracy of the estimates by introducing higher-order infinitesimals. Compared to the Euler-Maruyama method, the Milstein method is more precise. However, the Milstein method requires the stochastic process to be twice differentiable, which can make its implementation more complex. It is primarily suitable for stochastic differential equations with continuous sample paths. For stochastic differential equations with discontinuous sample paths or jump processes, other types of numerical methods may be required.

    Assuming an initial condition of (Sh(0),Ih(0),Rh(0),Sv(0),Iv(0),B(0))=(400,100,150,500, 120, 1000), the specific parameter values are as follows: Λ=35day1, Π=30day1, β1=0.004day1, β2=0.001day1, β3=0.003day1, β4=0.002day1, λh=0.1day1, δh=0.6day1, μh=0.01day1, μv=0.1day1, K=10cellsml1, k=0.5day1, α1=0.08cellsml1day1, α2=0.09cellsml1day1 and γh=0.7day1.

    Figures 2 and 3 demonstrate the specific time-varying situation of the number of infected individuals or infected vectors when these four parameters β3,δh,γh,μv change, while other parameters remain unchanged, respectively. From these two figures, it can be observed that despite changes in the parameters, both the infected population and the infected vectors ultimately go extinct, but the time of extinction differs. Specifically, as β3 decreases, the extinction time of Ih shortens. Similarly, when δh and γh increase, the extinction time of Ih decreases. Additionally, as μv increases, the extinction time of Iv also shortens.

    Figure 2.  Numerical simulations of deterministic and stochastic systems Ih under different β3 and δh. (a) and (c) represent the corresponding deterministic model of (1.1), while (b) and (d) represent the stochastic model (1.1).
    Figure 3.  Numerical simulations of deterministic and stochastic systems Ih and Iv under different γh and μv. (a) and (c) represent the corresponding deterministic model of (1.1), while (b) and (d) represent the stochastic model (1.1).

    In this section, we utilize the reported leptospirosis case data in China from 2003 to 2021 to predict the future epidemic situation of the disease. The data comes from China's statistical Yearbook [20], as shown in Figure 4. The population recruitment rate of Λ=7.74×106 is estimated based on China's population statistics from 2003 to 2021, the natural death rate of humans is μh=0.0064, and the number of newly reported leptospirosis cases in 2003 was 1728 [20]. Assuming that the recruitment rate of vectors carrying leptospira is Π=1.0812×105, these vectors are susceptible to external factors that can lead to death, with a natural death rate of μv=0.8125 [21]. The specific values of the parameters are listed in Table 1.

    Figure 4.  The Report on Leptospirosis Cases in China from 2003 to 2021.
    Table 1.  Parameter values and sources.
    Parameter Parameter value Source Parameter Parameter value Source
    Λ 7.74×106 year1 [20] Π 1.0812×105 year1 [22]
    [1mm] β2 1×105 year1 Fitted β4 1×105 year1 Fitted
    K 4.65×108 cellsml1 Fitted k 0.162 year1 [20]
    μh 0.0064 year1 [20] μv 0.8125 year1 [21]
    α1 3 cellsml1year1 [20] α2 100 cellsml1year1 Fitted
    λh 0.08082 year1 [21] δh 0.03328 year1 [23]
    γh 0.08889 year1 [23]

     | Show Table
    DownLoad: CSV

    Let the cumulative number of leptospirosis cases in the human population be defined as Dh(t), and

    dDh(t)dt=β1ShIvNh+β3ShBK+B. (3.1)

    To predict the disease, it is necessary to first estimate the two important parameters that affect the spread of the disease, namely, β1,β3. We utilize the numerical solution Dh(t) from model (3.1) to fit the data. Let Θ(β1,β3) represent the vector of parameters to be estimated, and Dh(t,Θ) represent the numerical solution of model (3.1) corresponding to the parameters Θ. The vector Y(Yk,k=1,2,3,...,19) represents the 19 statistical data points, and tk is the corresponding time for each data point. Take the initial value of the variable as (Sh(0),Ih(0),Rh(0),Sv(0),Iv(0),B(0),Dh(0))=(7.74×106,1728,307,1.0812×105,1.867×103,1.42×102,1728), and the initial value of the parameter (β1,β3)=(3.2326×103,1.2×104). Random disturbance intensities are taken as σ1=σ2=σ3=σ4=σ5=σ6=0.1. We estimate the parameters using two methods below: one is the least squares method, and the other is the Markov Chain Monte Carlo (MCMC) method.

    1) The least squares method (LSM). The goal is to find the optimal values of Θ(β1,β3) that minimize the least squares criterion:

    LS=19k=1|Dh(tk,Θ)Yk|2. (3.2)

    To achieve this, we utilize the fmincon command in the mathematical software MATLAB for numerical optimization. Based on the biological background, we set the ranges of Θ to be ((0,0),[0.5,0.5]), which serve as the constraint conditions. Using the optimization algorithm, we obtain the estimated values of the parameters. Then, we run the program 100 times and calculate the average of the output parameters β1=0.0032308,β3=0.00011993, which serve as the required parameter estimates. Figure 5(a), (b) present numerical simulations of the cumulative number of leptospirosis cases in 100 sample paths and their mean output path, respectively.

    Figure 5.  LSM analysis chart for parameters β1 and β3.

    2) Markov Chain Monte Carlo-Metropolis Hastings method (MCMC-MH). Now, we estimate the parameters using the MCMC parameter estimation method combined with MH sampling. Let Θ(β1,β3) be the proposed parameter and Θ(β1,β3) be the current parameter. The proposed parameter follows Θ=Θ+ε, where ε is the step size of random walk that follows a uniform distribution. According to Bayesian statistical inference, the posterior distribution is given by:

    P(Θ|Y)=L(Y|Θ)P(Θ), (3.3)

    where the likelihood function is L(Y|Θ)=19k=1|Dh(tk,Θ)Yk|2, and P(Θ) is the non-informative prior distribution, assumed to be a constant C. The acceptance probability is defined as: α(Θ,Θ)=min{1,exp(L(Y|Θ)L(Y|Θ))}. The ranges of Θ are also ((0,0), [0.5,0.5]). After performing 5000 iterations of MCMC calculations, with a burn-in period of 1000 iterations, we computed the average of the last 4000 iterations to obtain the estimated values of the parameters as β1=0.0050193,β3=0.000096193. The 95 percent confidence interval for β1 and β3 is (1.432×1039.941×103), (1.5036×1052.2604×104), respectively. By substituting the estimated parameters into the model (3.1), we can obtain any 100 paths of Dh(t). Figure 6(a), (b) present numerical simulations of the cumulative number of leptospirosis cases in 100 sample paths and their mean output path, respectively. Figure 6(c), (d) show the posterior distribution plots and trace plots for β1, β3, respectively.

    Figure 6.  MCMC analysis chart for parameters β1 and β3.

    It can be seen from Figures 5 and 6 that both simulation results of the model (3.1) by two methods match the cumulative data of leptospirosis cases in China from 2003 to 2021. Next, we calculate the error value between the average curve and the real data, and compare the results from both two methods. It can be seen from Table 2 that the parameter values estimated by the two methods are very close, but the estimation error by the MCMC-MH method is smaller than LSM. Finally, using the parameters estimated by the MCMC-MH method, we calculate the basic reproduction number for the transmission of leptospirosis in China, Rm0.00075197<1, and predict that leptospirosis will be eliminated in China in 26 years (see Figure 7).

    Table 2.  Error comparison.
    Method The estimated value of β1 The estimated value of β3 MAPE RSME
    LSM 0.0032308 0.00011993 0.6236 4190.7348
    MCMC 0.0050193 0.000096193 0.61821 3968.3587

     | Show Table
    DownLoad: CSV
    Figure 7.  Prediction chart of the future trend of leptospirosis.

    This article establishes a stochastic leptospirosis model with both vector and environmental transmission. Through mathematical analysis of the model, a threshold for disease elimination is derived. Then, using the partial rank correlation coefficient, an impact analysis was conducted on the model parameters to identify the key parameters that have a significant influence on disease elimination. Furthermore, a sensitivity analysis of these parameters was carried out through numerical simulations, which further revealed the mechanisms of their role in the disease transmission process. This analytical approach provides a powerful tool for gaining a deeper understanding of how model parameters affect disease transmission. In the end, using data from China's leptospirosis case reports from 2003 to 2021, two parameter estimation methods, LSM and MCMC-MH, are applied to estimate the crucial parameters of the model. The simulation results of the number of infections in model (1.1) using parameters obtained from two parameter estimation methods align well with the cumulative data of leptospirosis cases in China from 2003 to 2021. It is predicted that under the current control measures, leptospirosis in China will be completely eliminated after 26 years.

    Common leptospirosis models [3,5,22] tend to only consider the interaction between hosts and vectors, overlooking the influence of environmental factors. In this paper, by incorporating environmental transmission factors into the model design and considering environmental disturbance, we construct a more comprehensive and realistic stochastic infectious disease model, providing a new perspective for a more accurate understanding of the transmission mechanisms of leptospirosis. Specifically, the parameter estimation method used in this article, which combines MH sampling with MCMC, has served as a good demonstration for parameter estimation in stochastic differential systems with numerous parameters. This approach of combining actual data with parameter estimation not only enhances the accuracy and reliability of the model, but also provides strong support for predicting the future trends of leptospirosis in China. The stochastic model of leptospirosis and its related analysis methods established in this article have important theoretical and practical significance for understanding the transmission patterns of other similar vector-borne diseases and predicting future epidemic trends.

    However, it must be said that when we make predictions, we only estimate two important parameters, and some parameters are based on subjective assumptions fitted to the data, which may reduce the accuracy of the prediction. In addition, the model does not fully consider the impact of human behavior, socioeconomic factors, and climate change on disease transmission. The neglect of these factors may limit the accuracy and applicability of the model. In the future, we will incorporate human behavior, socioeconomic factors, and climate change into our model, and strive to utilize actual data to estimate more parameters in order to improve the accuracy and applicability of the model. This will help us gain a deeper understanding of the dynamics of disease transmission and design effective interventions to protect public health.

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

    This work is sponsored by Nanhu Scholars Program for Young Scholars of XYNU.

    The authors declare there is no conflicts of interest.



    [1] L. Aceto, H. R. Malonek, G. Tomaz, A unified matrix approach to the representation of Appell polynomials, Integr. Transf. Spec. F., 26 (2015), 426–441. doi: 10.1080/10652469.2015.1013035
    [2] L. Aceto, I. Caçāo, A matrix approach to Sheffer polynomials, J. Math. Anal. Appl., 446 (2017), 87–100. doi: 10.1016/j.jmaa.2016.08.038
    [3] L. Aceto, H. R. Malonek, G. Tomaz, Matrix approach to hypercomplex Appell polynomials, Appl. Numer. Math., 116 (2017), 2–9. doi: 10.1016/j.apnum.2016.07.006
    [4] M. Ali, T. Nahid, S. Khan, Some results on hybrid relatives of the Sheffer polynomials via operational rules, Miskolc Math. Notes, 20 (2019), 729–743. doi: 10.18514/MMN.2019.2958
    [5] S. Araci, M. Acikgoz, K. Park, H. Jolany On the unification of two families of multiple twisted type polynomials by using p-Adic q-integral at q=1, B. Malays. Math. Sci. So., 37 (2014), 543–554.
    [6] S. Araci, E. A˘gy¨uz, M. Acikgoz, On a q-analog of some numbers and polynomials, J. Inequal. Appl., 2015 (2015), 19. doi: 10.1186/s13660-014-0542-y
    [7] S. Araci, ¨O. ¨Ozer, Extended q-Dedekind-type Daehee-Changhee sums associated with extended q-Euler polynomials, Adv. Differ. Equ., 2015 (2015), 272. doi: 10.1186/s13662-015-0610-8
    [8] R. Askey, Orthogonal polynomials and special functions, Society for Industrial and Applied Mathematics, 1975.
    [9] L. Bedratyuk, N. Luno, Some properties of generalized hypergeometric Appell polynomials, Carpathian Math. Publ., 12 (2020), 129–137. doi: 10.15330/cmp.12.1.129-137
    [10] F. Costabile, F. DellAccio, M. I. Gualtieri, A new approach to Bernoulli polynomials, Rend. Mat., 26 (2006), 1–12.
    [11] F. A. Costabile, On expansion of a real function in Bernoulli polynomials and applications, Conferenze del Seminario Matem. Univ. Bari. (IT) n273, 1999.
    [12] F. A. Costabile, E. Longo, A determinantal approach to Appell polynomials, J. Comput. Appl. Math., 234 (2010), 1528–1542. doi: 10.1016/j.cam.2010.02.033
    [13] F. A. Costabile, E. Longo, An algebraic exposition of umbral calculus with application to general interpolation problem–A survey, Publ. I. Math., 96 (2014), 67–83. doi: 10.2298/PIM1410067C
    [14] F. A. Costabile, E. Longo, An algebraic approach to Sheffer polynomial sequences, Integr. Transf. Spec. F., 25 (2014), 295–311. doi: 10.1080/10652469.2013.842234
    [15] G. Dattoli, M. Migliorati, H. M. Srivastava, Sheffer polynomials, monomiality principle, algebraic methods and the theory of classical polynomials, Math. Comput. Model., 45 (2007), 1033–1041. doi: 10.1016/j.mcm.2006.08.010
    [16] S. Khan, T. Nahid, Certain results associated with hybrid rRelatives of the q-sheffer sequences, Bol. Soc. Paran. Mat., In press.
    [17] S. Khan, T. Nahid, Finding non-linear differential equations and certain identities for the Bernoulli-Euler and Bernoulli-Genocchi numbers, SN Appl. Sci., 1 (2019), 217. doi: 10.1007/s42452-019-0222-0
    [18] S. Khan, T. Nahid, Numerical computation of zeros of certain hybrid q-special sequences, Procedia Comput. Sci., 152 (2019), 166–171. doi: 10.1016/j.procs.2019.05.039
    [19] S. Khan, T. Nahid, Determinant forms, difference equations and zeros of the q-Hermite-Appell polynomials, Mathematics, 6 (2018), 258. doi: 10.3390/math6110258
    [20] S. Khan, N. Raza, 2-Iterated Appell polynomials and related numbers, Appl. Math. Comput., 219 (2013), 9469–9483.
    [21] N. Khan, T. Usman, J. Choi, A new class of generalized polynomials, Turk. J. Math., 42 (2018), 1366–1379.
    [22] N. U. Khan, T. Usman, A new class of Laguerre-based poly-Euler and multi poly-Euler polynomials, J. Anal. Num. Theor., 4 (2016), 113–120. doi: 10.18576/jant/040205
    [23] T. Kim, On the multiple q-Genocchi and Euler numbers, Russ. J. Math. Phys., 15 (2008), 481–486. doi: 10.1134/S1061920808040055
    [24] T. Kim, D. V. Dolgy, D. S. Kim, J. J. Seo, Differential equations for Changhee polynomials and their applications, J. Nonlinear Sci. Appl., 9 (2016), 2857–2864. doi: 10.22436/jnsa.009.05.80
    [25] T. Kim, D. S. Kim, A note on nonlinear Changhee differential equation, Russ. J. Math. Phys., 23 (2016), 88–92. doi: 10.1134/S1061920816010064
    [26] T. Kim, D. S. Kim, Differential equations associated with Catalan-Daehee numbers and their applications, RACSAM, 111 (2017), 1071–1081. doi: 10.1007/s13398-016-0349-4
    [27] D. S. Kim, T. Kim, Higher-order Bernoulli and poly-Bernoulli mixed type polynomials, Georgian Math. J., 22 (2015), 265–272.
    [28] D. S. Kim, T. Kim, Higher-order Cauchy of the first kind and poly-Cauchy of the first kind mixed type polynomials, Adv. Stud. Contemp. Math., 23 (2013), 621–636.
    [29] D. S. Kim, T. Kim, H. I. Kwon, J. J. Seo, Identities of some special mixed type polynomials, Adv. Stud. Theor. Phys., 8 (2014), 745–754. doi: 10.12988/astp.2014.4686
    [30] T. Kim, D. S. Kim, H. I. Kwon, J. J. Seo, Revisit nonlinear differential equations associated with Bernoulli numbers of the second kind, Glob. J. Pure Appl. Math., 12 (2016), 1893–1901.
    [31] D. S. Kim, T. Kim, J. J. Seo, S. H. Lee, Higher-order Changhee numbers and polynomials, Adv. Studies Theor. Phys., 8 (2014), 365–373. doi: 10.12988/astp.2014.4330
    [32] J. G. Lee, L. C. Jang, J. J. Seo, S. K. Choi, H. I. Kwon, On Appell-type Changhee polynomials and numbers, Adv. Differ. Equ., 2016 (2016), 160. doi: 10.1186/s13662-016-0866-7
    [33] M. Riyasat, S. Khan, T. Nahid, q-difference equations for the composite 2D q-Appell polynomials and their applications, Cogent Math., 4 (2017), 1376972. doi: 10.1080/23311835.2017.1376972
    [34] O. Ore, On a special class of polynomials, T. Am. Math. Soc., 35 (1933), 559–584. doi: 10.1090/S0002-9947-1933-1501703-0
    [35] M. Saif, R. Nadeem, Evaluation of Apostol–Euler based poly Daehee polynomials, Int. J. Appl. Comput. Math., 6 (2020), 1.
    [36] M. J. Schlosser, Multiple hypergeometric series: Appell series and beyond, In: Computer algebra in quantum field theory, Vienna: Springer, 2013.
    [37] H. M. Srivastava, H. L. Manocha, A treatise on generating functions, New York: Halsted Press, 1984.
    [38] P. Tempesta, On Appell sequences of polynomials of Bernoulli and Euler type, J. Math. Anal. Appl., 341 (2008), 1295–1310. doi: 10.1016/j.jmaa.2007.07.018
  • This article has been cited by:

    1. Habib ur Rehman, Wiyada Kumam, Poom Kumam, Meshal Shutaywi, A new weak convergence non-monotonic self-adaptive iterative scheme for solving equilibrium problems, 2021, 6, 2473-6988, 5612, 10.3934/math.2021332
    2. Chainarong Khanpanuk, Nuttapol Pakkaranang, Nopparat Wairojjana, Nattawut Pholasa, Approximations of an Equilibrium Problem without Prior Knowledge of Lipschitz Constants in Hilbert Spaces with Applications, 2021, 10, 2075-1680, 76, 10.3390/axioms10020076
    3. Charu Batra, Nishu Gupta, Renu Chugh, Rajeev Kumar, Generalized viscosity extragradient algorithm for pseudomonotone equilibrium and fixed point problems for finite family of demicontractive operators, 2022, 68, 1598-5865, 4195, 10.1007/s12190-022-01699-x
    4. Pongsakorn Yotkaew, Nopparat Wairojjana, Nuttapol Pakkaranang, Accelerated non-monotonic explicit proximal-type method for solving equilibrium programming with convex constraints and its applications, 2021, 6, 2473-6988, 10707, 10.3934/math.2021622
    5. Olawale Kazeem Oyewole, Simeon Reich, An Inertial Subgradient Extragradient Method for Approximating Solutions to Equilibrium Problems in Hadamard Manifolds, 2023, 12, 2075-1680, 256, 10.3390/axioms12030256
    6. Nopparat Wairojjana, Chainarong Khunpanuk, Nuttapol Pakkaranang, Strong convergence analysis of modified Mann-type forward–backward scheme for solving quasimonotone variational inequalities, 2023, 16, 1793-5571, 10.1142/S1793557123500912
  • Reader Comments
  • © 2021 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

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

Metrics

Article views(2138) PDF downloads(90) Cited by(2)

Figures and Tables

Figures(8)

Other Articles By Authors

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog