<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2013.44091</article-id><article-id pub-id-type="publisher-id">AM-30436</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  The Effects of a Backward Bifurcation on a Continuous Time Markov Chain Model for the Transmission Dynamics of Single Strain Dengue Virus
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>dnan</surname><given-names>Khan</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Muhammad</surname><given-names>Hassan</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mudassar</surname><given-names>Imran</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Centre for Advanced Studies in Mathematics, Lahore University of Management Sciences, Lahore, Pakistan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>mudassar.imran@lums.edu.pk(MI)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>16</day><month>04</month><year>2013</year></pub-date><volume>04</volume><issue>04</issue><fpage>663</fpage><lpage>674</lpage><history><date date-type="received"><day>February</day>	<month>19,</month>	<year>2013</year></date><date date-type="rev-recd"><day>March</day>	<month>4,</month>	<year>2013</year>	</date><date date-type="accepted"><day>March</day>	<month>11,</month>	<year>2013</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   Global incidence of dengue, a vector-borne tropical disease, has seen a dramatic increase with several major outbreaks in the past few decades. We formulate and analyze a stochastic epidemic model for the transmission dynamics of a single strain of dengue virus. The stochastic model is constructed using a continuous time Markov chain (CTMC) and is based on an existing deterministic model that suggests the existence of a backward bifurcation for some values of the model parameters. The dynamics of the stochastic model are explored through numerical simulations in this region of bistability. The mean of each random variable is numerically estimated and these are compared to the dynamics of the deterministic model. It is observed that the stochastic model also predicts the co-existence of a locally asymptotically stable disease-free equilibrium along with a locally stable endemic equilibrium. This co-existence of equilibria is important from a public health perspective because it implies that dengue can persist in populations even if the value of the basic reproduction number is less than unity. 
 
</p></abstract><kwd-group><kwd>Epidemiology; Dengue Fever; Backward Bifurcation; Stochastic Model</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Dengue, a vector transmitted disease, has seen a dramatic increase in global incidence over the past decades [1,2]. Originally restricted to a handful of countries, dengue &#160;is now endemic in more than a hundred tropical and subtropical countries worldwide [1-3]. With an estimated &#160;50 - 100 million cases and nearly 10,000 - 20,000 deaths annually, dengue ranks second to Malaria amongst deadly mosquito-born diseases [1,2,4-6]. The disease is caused by one of four virus serotypes (strains) of the genus Flavivirus [2,3,7]. Most infected individuals suffer from dengue fever, a severe flu-like illness characterized by high fever, which poses only a limited threat to mortality [2,8]. The symptoms usually last for one to two weeks, after an initial incubation period of about 4 - 7 days [<xref ref-type="bibr" rid="scirp.30436-ref9">9</xref>]. A minority of infected individuals however, develops dengue hemorrhagic fever (DHF) resulting in bleeding, low levels of blood platelets and blood plasma leakage, or dengue shock syndrome (DSS) resulting in extremely low blood pressures. The risk associated with DHF and DSS is considerably higher, with mortality ranging from 5% - 15% [3,5,9,10].</p><p>Dengue is transmitted to humans through mosquito bites. Female mosquitos of the Aedas genus, primarily Aedas aegypti, acquire the dengue virus through a blood meal from infected humans [2,11]. The dengue virus has an incubation period of about 7 - 10 days in the vector, and is then spread to susceptible humans who are bitten by the infected mosquito [<xref ref-type="bibr" rid="scirp.30436-ref9">9</xref>]. The virus also has an incubation period of 4 - 7 days in the host [<xref ref-type="bibr" rid="scirp.30436-ref9">9</xref>]. While vectors never recover from infection with the dengue virus, the infection in hosts lasts only about one to two weeks [<xref ref-type="bibr" rid="scirp.30436-ref2">2</xref>]. Recovery from infection with one serotype of the dengue virus gives life-long immunity to that serotype but only temporary and partial immunity to other serotypes [2,4, 12-14]. Secondary infection with a different serotype may result in Antibody Dependent Enhancement (ADE), which is speculated to increase the chances of DHF and DSS [4,12,13,15]. In this study however, we will consider infection involving only a single serotype of the dengue virus.</p><p>Historical records indicate the occurrence of dengue epidemics in North America, Asia and Africa in the late 18th century [<xref ref-type="bibr" rid="scirp.30436-ref3">3</xref>]. Since then and up until the middle of the 20th century, incidences of dengue fever have been rare [<xref ref-type="bibr" rid="scirp.30436-ref3">3</xref>]. Since the 1970’s however, there has been a marked increase in the number of dengue cases, as well as dengue epidemics, with the WHO claiming a 30-fold increase in the incidence of dengue between 1960 and 2010 [2,3,8]. This dramatic increase is attributed to rapid urbanization, population growth and increase international travel [<xref ref-type="bibr" rid="scirp.30436-ref8">8</xref>]. Dengue disease is currently endemic in nearly 110 countries in Southeast Asia, the Americas, Africa and the Eastern Mediterranean [<xref ref-type="bibr" rid="scirp.30436-ref2">2</xref>]. It is estimated by the WHO, that nearly 2.5 billion people are at risk of contracting the disease. Furthermore, nearly 50 - 100 million cases and almost 20,000 deaths due to more severe forms of dengue fever are reported globally every year, making dengue one of the deadliest mosquitotransmitted diseases [1,2,4-6].</p><p>The dengue virus (DENV), which causes dengue fever in humans, is a single positive-stranded RNA virus of the family Flaviviridae and genus Flavivirus [2,3,7]. The virus has four distinct serotypes, DENV1, DENV2, DENV3 and DENV4, each of which can cause the full spectrum of the disease [2,3,7]. Owing to the difficulty of developing an immunization against all four serotypes, there is currently no vaccine against the disease [6,8], [<xref ref-type="bibr" rid="scirp.30436-ref11">11</xref>]. Infection with and recovery from a particular serotype of the dengue virus grants life-long immunity to that serotype but only gives temporary and/or partial immunity to the other serotypes [<xref ref-type="bibr" rid="scirp.30436-ref2">2</xref>]. This partial cross-immunity is the cause of antibody-dependent enhancement (ADE) in the setting of a secondary infection with a different serotype of DENV. ADE is hypothesized to be one factors leading to DHF and DSS, the more severe form of dengue disease [4,12,13,15].</p><p>The clinical symptoms and effects of dengue disease vary greatly. Nearly 80% of individuals suffering from a primary infection with DENV are asymptomatic or display only a mild, uncomplicated fever [2,8]. A minority of infected individuals suffer from DHF and DSS, the more severe forms of dengue disease [3,5,9]. As mentioned previously however, risk of DHF and DSS is associated primarily with secondary infection with a heterologous serotype of DENV [4,12,13,15]. In general, dengue disease is marked by three separate phases: febrile, critical and recovery. The characteristic symptoms of dengue in the febrile phase are the sudden onset of high fever, rash, headaches and muscle and joint pains, which lead to the alternative name “breakbone fever” for dengue disease [<xref ref-type="bibr" rid="scirp.30436-ref8">8</xref>]. This phase of the disease is rarely life threatening and the associated mortality is quite low. Most individuals then progress to the recovery phase. However, a minority of individuals first pass through the critical phase of the disease. This phase lasts for one or two days and is marked by low blood pressure, leakage of blood plasma from the capillaries and decreased blood supply to organs. Severe cases of these symptoms are associated with DHF and DSS and the mortality in this phase of the disease is estimated to be as high as 5% - 15% [3,5,8,9].</p><p>Over the past several years, a number of deterministic mathematical models have been proposed to analyze the transmission dynamics of dengue in urban communities [5,11-17]. L. Esteva and C. Vargas [<xref ref-type="bibr" rid="scirp.30436-ref14">14</xref>] have investigated the coexistence of two serotypes of dengue virus using a deterministic ODE model. Moreover, Ferguson et al. [<xref ref-type="bibr" rid="scirp.30436-ref15">15</xref>] have investigated the effects of ADE on the transmission of multiple serotypes of dengue virus. In addition, Garba et al. [<xref ref-type="bibr" rid="scirp.30436-ref11">11</xref>] have shown the existence of a backward bifurcation in a standard incidence ODE model for a single strain of dengue virus. Garba et al. [<xref ref-type="bibr" rid="scirp.30436-ref12">12</xref>] have also explored the effects of cross-immunity on the transmission dynamics of two strains of dengue virus. Similarly, H. Wearing and P. Rohani [<xref ref-type="bibr" rid="scirp.30436-ref13">13</xref>] have investigated the effects of both ADE and cross immunity on multiple serotypes of dengue virus. Finally, Chowel et al. [<xref ref-type="bibr" rid="scirp.30436-ref18">18</xref>] have estimated the basic reproduction number for dengue using spatial epidemic data.</p><p>In addition, over the past few decades, several stochastic epidemic models for the spread of infectious diseases have also been proposed and analyzed [19-27]. An important qualitative difference between deterministic and stochastic epidemic models in general is the asymptotic dynamics [<xref ref-type="bibr" rid="scirp.30436-ref28">28</xref>]. Furthermore, stochastic models also allow for the possibility of disease extinction in finite time and therefore the expected time to disease extinction can be calculated [19,28,29]. It is also observed that stochastic models better capture the uncertainty and variability that is inherent in real-life epidemics due to factors such as the unpredictability of person-to-person contact [27, 29]. L. J. S. Allen [28,29] has explored the utility of stochastic epidemic models by comparing them with deterministic models. Despite, the utility of stochastic models, however, very little stochastic modeling has been performed for the transmission dynamics of dengue virus (see [<xref ref-type="bibr" rid="scirp.30436-ref26">26</xref>] and the references therein).</p><p>The purpose of this study is to formulate and analyze a stochastic model for the transmission dynamics of a single strain of dengue virus using a continuous time Markov chain (CTMC). The stochastic model is based on an existing deterministic model proposed by Garba et al. [<xref ref-type="bibr" rid="scirp.30436-ref11">11</xref>] with one minor but nevertheless important difference: contrary to the original deterministic model [<xref ref-type="bibr" rid="scirp.30436-ref11">11</xref>] and in line with previous studies of dengue virus such as [12,13], we will assume that exposed hosts and exposed vectors do not transmit the disease. In addition, the deterministic model [<xref ref-type="bibr" rid="scirp.30436-ref11">11</xref>] postulates the existence of a backward bifurcation for a subset of the model parameters space. Therefore, a major aim of this study is to estimate the mean of each random variable in this region of bistability using numerical simulations. These will be compared to the dynamics of the deterministic model [<xref ref-type="bibr" rid="scirp.30436-ref11">11</xref>]. A previous study on the effect of a backward bifurcation on the dynamics of a stochastic epidemic model is given in [<xref ref-type="bibr" rid="scirp.30436-ref26">26</xref>].</p><p>This paper is organized as follows. The second section contains a description of the deterministic model formulated in [<xref ref-type="bibr" rid="scirp.30436-ref11">11</xref>] along with a discussion of the basic reproduction number <img src="10-7401382\399c0ae1-23c1-4d30-af15-9cc92e4b7eca.jpg" /> of the model as well as the conditions for the existence of the backward bifurcation. In Section 3 we formulate the stochastic model as a continuous time Markov chain (CTMC) and discuss some basic properties of the stochastic model. Finally, Section 4 contains the numerical simulations of the stochastic model. We conclude the paper by presenting a discussion of various directions in which to extend the current study.</p></sec><sec id="s2"><title>2. The Deterministic Model</title><sec id="s2_1"><title>2.1. Model Formulation</title><p>The deterministic model we have considered is a deterministic vector-host ODE model that assumes a homogenous mixing of the host (human) and vector (mosquito) populations. The total human population at time t, denoted by<img src="10-7401382\3b292229-d0cf-4342-966b-724d971b9a00.jpg" />, is divided into four mutually exclusive classes comprising of susceptible humans<img src="10-7401382\6c80ed2e-6955-4d11-85a3-1f9b83155dd4.jpg" />, exposed humans<img src="10-7401382\9f005241-fb11-421a-a986-9434323b48e8.jpg" />, infected humans <img src="10-7401382\cb5da399-82c1-4a7a-9d7c-39484c6aa5a4.jpg" /> and recovered humans<img src="10-7401382\b481c8d6-56f4-4362-9d59-b2aa6ec3715f.jpg" />. It is assumed that individuals who recover from infection with a particular serotype of Dengue gain lifelong immunity to it [<xref ref-type="bibr" rid="scirp.30436-ref12">12</xref>]. Similarly, the total vector population at time t is denoted by <img src="10-7401382\fdcebdd1-e0eb-4acd-9d86-8cad63fb120b.jpg" /> and is divided into three mutually exclusive classes comprising susceptible of susceptible vectors<img src="10-7401382\c67ba439-7be4-4547-a1c4-1ef776f838e0.jpg" />, exposed vectors <img src="10-7401382\dd157707-046b-4c1b-9b0c-6f9af08dc03c.jpg" /> and infected vectors<img src="10-7401382\77260048-34ab-4ecc-a9d5-e43ba4445c7e.jpg" />. It is assumed that vectors (mosquitoes) infected with a particular serotype of Dengue never recover [<xref ref-type="bibr" rid="scirp.30436-ref12">12</xref>]. As mentioned previously in the introduction, we will modify the original model of Garba et al. [<xref ref-type="bibr" rid="scirp.30436-ref11">11</xref>] by assuming that exposed humans and exposed vectors do not transmit the disease.</p><p>The model assumes that the susceptible human population <img src="10-7401382\fdd78947-a2eb-4147-bf36-9e2ae5cc11e4.jpg" /> has a constant recruitment rate <img src="10-7401382\5819be58-2914-4f54-b926-e96ae89b2514.jpg" /> and natural death rate<img src="10-7401382\e6f77bea-b9e1-4ecd-b769-362a529413b2.jpg" />. Susceptible individuals are infected with Dengue virus (due to contact with infected vectors) at a rate <img src="10-7401382\d9305970-be71-4528-81a6-4caab1fd196c.jpg" /> and thus enter the exposed class E<sub>H</sub>. The exposed population <img src="10-7401382\9627921b-1bdf-45e9-9834-7b150a30ea8b.jpg" /> is depleted at the natural death rate<img src="10-7401382\67364052-cc3f-422d-a0e5-ca7320107834.jpg" />. Additionally, exposed individuals develop symptoms and move into the infected class I<sub>H</sub> at a rate<img src="10-7401382\8014186b-5ad9-4868-83e5-49de2c96dbc7.jpg" />. The infected population <img src="10-7401382\e61ccf73-b8b1-4f75-af98-f13c7808602d.jpg" /> is depleted via the natural death rate mu, the disease-induced death rate <img src="10-7401382\aeca5d38-b39d-4fae-8263-aafeaa0168fb.jpg" /> and the recovery rate of infected individuals<img src="10-7401382\2eab3d5c-c62b-47cc-b730-af204d32993e.jpg" />. Finally, the recovered population <img src="10-7401382\2d757571-3cf9-40ed-ac8f-28283f029e3e.jpg" /> decreases due to the natural death rate mu.</p><p>Similarly, the susceptible vector population <img src="10-7401382\908be167-a3ad-41aa-a828-af477b4eca8b.jpg" /> has a constant recruitment rate <img src="10-7401382\2829e751-e38f-44ef-959f-4d46b8f72737.jpg" /> and a natural death rate<img src="10-7401382\4c1dfe2b-a712-4a3b-a282-e238d4ff674a.jpg" />. Susceptible vectors are infected with Dengue virus (due to effective contact with infected humans) at a rate <img src="10-7401382\12c233e2-5ef4-43f5-8eca-e471e3a47578.jpg" /> and thus move to the exposed vector class<img src="10-7401382\d6e54834-c8c0-4312-bfad-b4400aa638ae.jpg" />. The exposed vector class <img src="10-7401382\bf4f15c2-a2e9-4cf1-bb9b-d093d5a8baa6.jpg" /> is depleted at the natural death rate<img src="10-7401382\3bd68707-e326-41f8-ab3d-e880e5974112.jpg" />. In addition exposed vectors develop symptoms and move to the infected vector class <img src="10-7401382\4e79f7c6-355e-4c78-acdd-d32ad1be73fd.jpg" /> at a rate<img src="10-7401382\6cf268ba-3215-4062-bd8f-a55ec31e1f19.jpg" />. Infected vectors, in addition to the natural death rate <img src="10-7401382\769f6e9c-18b2-4398-a817-78203208508d.jpg" /> die at a disease induced death rate<img src="10-7401382\49af03c3-b127-49fe-a45b-913a414fccf6.jpg" />.</p><p>Mathematically, the modified determinstic model is as follows:</p><disp-formula id="scirp.30436-formula19175"><label>(2.1)</label><graphic position="anchor" xlink:href="10-7401382\e7effe17-6a92-45b2-813d-71c0e8f73e39.jpg"  xlink:type="simple"/></disp-formula><p>where,</p><p><img src="10-7401382\b9ac108e-2aaa-462d-9ccb-cbc81efee161.jpg" /></p><p>The basic reproduction number for the model (2.1) can be calculated using the next generation operator method given in [<xref ref-type="bibr" rid="scirp.30436-ref30">30</xref>]. Hence, for the model (2.1), <img src="10-7401382\6fd5cec2-b640-4d8d-a091-119759b5a4b0.jpg" />is given by</p><disp-formula id="scirp.30436-formula19176"><label>(2.2)</label><graphic position="anchor" xlink:href="10-7401382\05d753d9-fb22-47df-b52b-4743cec23dd3.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="10-7401382\1867b218-b275-4474-b8b9-95c2b89c0e31.jpg" />, <img src="10-7401382\9d72bd7d-d893-41ed-b524-06e4c32c2d60.jpg" />, <img src="10-7401382\f464c936-27d7-464b-bd3c-3d89f23f1b5a.jpg" />and<img src="10-7401382\2b1ed4e3-ded9-43a4-aef1-4f13f4b09cb1.jpg" />.</p><p>It follows from [<xref ref-type="bibr" rid="scirp.30436-ref30">30</xref>] that the following lemma holds.</p><p>Lemma 1. The system (2.1) has a locally asymptotically stable disease-free equilibrium (DFE) given by</p><p><img src="10-7401382\1cc4aba9-0f99-4b28-a324-4b570fc3c833.jpg" />, whenever<img src="10-7401382\e8a1133c-3225-4a82-9f77-9b714f4bf6ce.jpg" />. The DFE given by <img src="10-7401382\fe03fe39-70ea-41ea-973c-1941e0ac9eb8.jpg" /> is locally unstable whenever<img src="10-7401382\4727b058-5359-432d-94f0-0e88c7cb0e21.jpg" />.</p><p>It should be pointed out however, that we have not proven that the DFE is globally asymptotically stable for values of the basic reproduction number<img src="10-7401382\63e56cba-e4c0-49ca-b227-cdaea0ba4ec5.jpg" />. Indeed, as shown in the next section, this is not true.</p></sec><sec id="s2_2"><title>2.2. Backward Bifurcation</title><p>As mentioned in the introduction, Garba et al. proved that the deterministic model presented in [<xref ref-type="bibr" rid="scirp.30436-ref11">11</xref>] undergoes a backward bifurcation for certain values of the model parameters. Since the model (2.1) considered in this study is a special case of the model considered by Garba et al. in [<xref ref-type="bibr" rid="scirp.30436-ref11">11</xref>], it follows easily that model (2.1) also undergoes a backward bifurcation. This is detailed in Theorem 1.</p><p>Theorem 1. Define the constants <img src="10-7401382\b4289a87-9bc1-4e9c-a2ab-f7729cbe56de.jpg" /> and <img src="10-7401382\5b5d3999-66d4-429d-86b7-8138c9f1eea6.jpg" /> as follows:</p><p><img src="10-7401382\06f5da2a-6699-4ed8-8643-35552638d892.jpg" /></p><p><img src="10-7401382\0d0187d0-e1a5-4aa7-aa6f-e9c1ed92fb69.jpg" /></p><p><img src="10-7401382\4e471183-2aae-47d1-8001-6529af152956.jpg" /></p><p>Then, the system (2.1) has:&#160;</p><p>• A unique endemic equilibrium if<img src="10-7401382\517cff08-323e-413e-8e76-5ec0a672e007.jpg" />.</p><p>• A unique endemic equilibrium if<img src="10-7401382\1e96f56c-5c66-439a-8295-639891215cb7.jpg" />, and <img src="10-7401382\20e9cbb7-487f-416c-813c-aaa47f2e3498.jpg" /> or<img src="10-7401382\3e4d17d5-21d4-439b-840e-dab7ee136ff8.jpg" />.</p><p>• Two endemic equilibria if <img src="10-7401382\5b64a2a0-9313-48ae-8a2c-958f2785d676.jpg" /> and <img src="10-7401382\f1870bd8-7de6-44b4-b72e-34c1bac6d315.jpg" />.</p><p>• No endemic equilibrium otherwise.</p><p>Furthermore, if case 3) from above holds and we define <img src="10-7401382\e3210d6b-0349-43b8-bf51-543e747c2dd0.jpg" /> as follows</p><disp-formula id="scirp.30436-formula19177"><label>(2.3)</label><graphic position="anchor" xlink:href="10-7401382\d3838af3-41be-4140-8fc9-6dd7febea372.jpg"  xlink:type="simple"/></disp-formula><p>then a backward bifurcation of the system (2.1) occurs for values of the basic reproduction <img src="10-7401382\e908fb92-a1a7-448a-b0e2-e04200bd083d.jpg" /> such that</p><p><img src="10-7401382\31e691e2-5d49-477c-94c9-a6c0a7749705.jpg" />.</p><p>Proof. By setting<img src="10-7401382\74f20b5e-62de-4497-80a6-7345935010ac.jpg" />, the result follows readily from the proof of Theorem 1 in [<xref ref-type="bibr" rid="scirp.30436-ref11">11</xref>].</p><p>As a consequence of Theorem 1, the model (2.1) does not possess a globally asymptotically stable DFE for<img src="10-7401382\ce810143-321e-4ad6-9ff4-7c167656e1bc.jpg" />. Indeed, it is clear that for certain values of<img src="10-7401382\364fe78a-d8c9-45bb-b9ee-1a32ce3eca37.jpg" />, there is a simultaneous co-existence of a locally asymptotically stable DFE alongside a locally asymptotically stable endemic equilibrium. Thus, lowering the value of the basic reproduction number <img src="10-7401382\5e441d8c-e1db-45dc-98ad-7bc55857fceb.jpg" /> to less than unity is no longer a sufficient condition to ensure disease elimination. From an epidemiological perspective, this possibility is extremely important because it implies that the dengue virus can persist in a population even when<img src="10-7401382\c893b4f4-cdd2-47b0-ba9d-291022651a7b.jpg" />.</p></sec></sec><sec id="s3"><title>3. The Stochastic Model</title><p>We now formulate an analogous stochastic model using a continuous time Markov chain. Our main purpose in this study will be to explore the dynamics of the stochastic model using numerical simulations in the region of bistability predicted by Theorem 1 and compare them to the corresponding results from the deterministic model (2.1). It has been observed [<xref ref-type="bibr" rid="scirp.30436-ref25">25</xref>] that for epidemic models exhibiting backward bifurcation, the deterministic and stochastic versions of the model do not always have similar dynamics. This difference is all the more important since, it is also observed that stochastic models better capture the uncertainty and variability that is inherent in real-life epidemics due to factors such as the unpredictability of person-to-person contact [27,28].</p>Model Formulation<p>Following [<xref ref-type="bibr" rid="scirp.30436-ref29">29</xref>], we assume the total population size to be bounded. We denote the bound by K. Let<img src="10-7401382\7e5b281c-48ff-49eb-86b7-4e6c684e3449.jpg" />, <img src="10-7401382\3efa788f-9710-4096-99ed-7d8cfbb17fff.jpg" />and <img src="10-7401382\4b21c964-b740-48d3-aeaf-42e6c746741d.jpg" /> denote discrete random variables for the number of susceptible hosts, exposed hosts, infected hosts, recovered hosts, susceptible vectors, exposed vectors and infected vectors respectively. Furthermore, let <img src="10-7401382\b6f1566a-e840-4e17-8dcd-5e69667a9abb.jpg" /> and</p><p><img src="10-7401382\b80ad014-ada6-45cc-92cc-caeb7670a38f.jpg" /></p><p>with</p><p><img src="10-7401382\463c787d-9bee-452b-b4ac-25f615f00b6f.jpg" /></p><p>The continous-time stochastic dynamical system</p><p><img src="10-7401382\6db4b73f-bd52-4a05-9ffa-a0f779eec6d4.jpg" /></p><p>is a multivariate process with a joint probability function with</p><disp-formula id="scirp.30436-formula19178"><label>(3.1)</label><graphic position="anchor" xlink:href="10-7401382\044d4ff9-9307-434a-870f-8c4fafeecf51.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="10-7401382\6a8966cb-04ba-44ef-a46f-d079beb47d8d.jpg" />and<img src="10-7401382\8c2cba8c-c931-4478-9e79-08e2cf5a52a0.jpg" />.</p><p>We further assume that the stochastic process is time homogeneous. Thus, using the notation of [<xref ref-type="bibr" rid="scirp.30436-ref28">28</xref>],</p><p><img src="10-7401382\d8cfa97b-3aea-4c83-932d-91a029ba3a97.jpg" />and therefore, the probability of transition from the state <img src="10-7401382\c80144eb-c8e5-4d64-80db-28ee860caaac.jpg" /> to the state</p><p><img src="10-7401382\a7f59c8b-2ebd-4255-bbd7-44db1411647c.jpg" /></p><p>is defined by</p><p><img src="10-7401382\9d09f952-b31a-45b9-96fb-cd136cd34680.jpg" /></p><p>where</p><p><img src="10-7401382\4248fe36-042f-41cc-8212-525cb4be3696.jpg" /></p><p>In order for the probabilities to be meaningful (non-negative and bounded by 1), the following is assumed:</p><p><img src="10-7401382\6509d63e-ef5b-4e9e-af6e-107ab4d86a24.jpg" />.</p><p>Since all the parameters are positive, a small value of <img src="10-7401382\9ccbe5ab-54a9-4dd0-a333-d1baed36c966.jpg" /> ensures that the above condition is satisfied.</p><p>Although, we now have the infinitesimal transition probabilities in hand, it is difficult to express the transition matrix and the generator matrix in easily expressible forms. One possible solution to this problem is given in [<xref ref-type="bibr" rid="scirp.30436-ref19">19</xref>] and we will make use of this later. Our stochastic model has seven independent discrete random variables and it is therefore even more cumbersome to express the associated transition and generator matrices. We therefore desist from this exercise for now.</p><p>We now assume that the stochastic process satisfies the Markov property [<xref ref-type="bibr" rid="scirp.30436-ref28">28</xref>]:</p><p><img src="10-7401382\acba7ab3-7338-416b-9b8e-7a95f940f749.jpg" /></p><p>Using the Markov property and the infinitesimal transition probabilities, we can express the state probabilities at time <img src="10-7401382\5aaba7b1-0b3a-47c7-8a0b-c5da00caaf2d.jpg" /> in terms of the state probabilities at time t. For the sake of simplicity, we assume that the total population at time t is less than the upper bound K and furthermore that none of the random variables is zero. The purpose of these two assumptions is to ignore numerous tedious sub-cases.</p><p>Proposition 1. Assume<img src="10-7401382\53271b79-54d7-4c98-b25a-deedd4e93ce3.jpg" />. Further assume that none of the variables s<sub>h</sub>, e<sub>h</sub>, i<sub>h</sub>, r, s<sub>v</sub>, e<sub>v</sub>, i<sub>v</sub> is zero. Then, the state probabilities <img src="10-7401382\2b4c1cec-5d8a-4ed3-aca9-00ccbbaf1adb.jpg" /> satisfy the following difference equations</p><p><img src="10-7401382\c86767e3-8873-4117-a2db-9f7fc9ef1926.jpg" /></p><p>where <img src="10-7401382\8614e2c2-239e-49a2-b6ec-cb77f3d0877f.jpg" /></p><p>The remaining cases, which result from removing the previous assumptions, are straightforward to calculate.</p><p>Some properties of the Markov chain can now be discussed. The Markov chain is reducible, with two important communication classes [<xref ref-type="bibr" rid="scirp.30436-ref28">28</xref>], given by</p><p><img src="10-7401382\4ca61107-6705-4517-be12-980fb0946c7f.jpg" /></p><p>and</p><p><img src="10-7401382\712a9ede-8423-4bdc-8795-88d8b953e887.jpg" /></p><p>Furthermore, E is not closed since, for example,<img src="10-7401382\824a30f4-8416-47ae-9beb-e21f2610ddd1.jpg" />. On the other hand, D is closed since</p><p><img src="10-7401382\4e0d6be3-acc1-4889-9038-0fecf8f9115b.jpg" /></p><p>Since E is an open class, all states in E are transient. Hence and in view of D being the only closed communication class, all sample paths will eventually be absorbed into the communication class D. However, while D is indeed a closed class, it does not contain an absorbing state since <img src="10-7401382\5b21d291-d0a5-48ee-b3fe-064ce6bd2ce8.jpg" /> <img src="10-7401382\33bbbb7d-b4f0-4262-9abf-fdf0cc36a552.jpg" />, <img src="10-7401382\c8833989-862a-465f-98dc-7fd300ab11f3.jpg" /></p><p>In view of the above discussion, the following theorem is established.</p><p>Theorem 2. The CTMC is a reducible chain with no absorbing states. However, all sample paths are eventually absorbed in the closed class</p><p><img src="10-7401382\7e309a4f-193e-4245-a316-891a239af869.jpg" />.</p><p>The two communication classes D and E correspond to the disease-free and endemic stages of the disease respectively. Therefore, the above result indicates that every sample path is eventually absorbed into the disease-free class and therefore, irrespective of parameter values, the stochastic model will always converge to a disease-free state. This is in direct contrast to the deterministic case in which a unique endemic steady state solution always exists for<img src="10-7401382\d445fb30-cf8d-40d0-8b3c-7355011120af.jpg" />. Thus, the deterministic case allows for the possibility of the disease having an endemic equilibrium, depending on the value of a threshold parameter, while the stochastic model always predicts an eventual disease-free equilibrium. Furthermore, disease extinction takes place in finite time in the stochastic case while in the deterministic case a disease-free equilibrium is only approached asymptotically. Depending on the value of <img src="10-7401382\f35c3a5c-338d-41d4-afbb-81b7f0c8dd33.jpg" /> however, the sample paths for the stochastic model might remain in the endemic class E for a very long time. As a consequence, for most practical purposes, the stochastic model follows closely the behavior of the corresponding deterministic model for the majority of time. This can be demonstrated using numerical simulations.</p></sec><sec id="s4"><title>4. Numerical Simulations</title><p>Our purpose in this section is to explore the dynamical behavior of the stochastic model for values of the model parameter, which result in a backward bifurcation and produce a region of bistability. The behavior of the stochastic model in this region is important due to the public health implications of the backward bifurcation. As mentioned previously, the existence of a backward bifurcation in model (2.1) results in the possibility of a locally asymptotically stable endemic equilibrium even for values of<img src="10-7401382\d74781f6-7250-45af-9e9d-60a1f269b7f0.jpg" />. Therefore, lowering the value of the basic reproduction number below unity is no longer a sufficient condition for disease elimination. Moreover, as mentioned in [<xref ref-type="bibr" rid="scirp.30436-ref25">25</xref>], the dynamics of a stochastic epidemic model does not necessarily agree with its deterministic counterpart in this region of bistability.</p><p>For the purpose of numerical simulations, we will formulate our stochastic model as a discrete time Markov chain (DTMC) and employ a constant time step<img src="10-7401382\1959d31d-28db-4a9a-be98-e78f60fe948a.jpg" />. This simplifies many of the numerical simulations and allows us to calculate the numerical mean, which is not possible when using a CTMC with random, exponentially distributed interevent times. As mentioned in [<xref ref-type="bibr" rid="scirp.30436-ref19">19</xref>], if the time step <img src="10-7401382\8c68a526-ff98-481c-9be8-c2215a487e76.jpg" /> is small enough, the DTMC provides an excellent approximation to the original formulation of the stochastic model as CTMC.</p><p>For the numerical simulations in this section, the following parameter values were chosen [<xref ref-type="bibr" rid="scirp.30436-ref11">11</xref>]:</p><p><img src="10-7401382\9530b80a-6312-4475-bc53-ec65e93924f0.jpg" /></p><p>This results in a value of R<sub>0</sub> = 0.855 and R<sub>c</sub> = 0.571 and thus we have<img src="10-7401382\1066035c-3c7d-41c2-b45c-d5134b079276.jpg" />. Therefore, in view of Lemma 1 and Theorem 1, the deterministic model (2.1) now has a locally asymptotically stable disease-free equilibrium (DFE) as well as a locally asymptotically stable endemic equilibrium. We point out however, that these parameter values are not necessarily realistic from a biological and epidemiological point of view.</p><p>We numerically simulate 500 sample paths to estimate the mean of each discrete random variable<img src="10-7401382\8e705e88-11fc-42e2-8c31-ddb8e683ca00.jpg" />,<img src="10-7401382\4307927c-5203-46fb-b922-ad03b863bb7b.jpg" />. The following initial conditions were chosen:</p><p>Initial Population:</p><p><img src="10-7401382\4660f526-a1df-4e09-90db-cf42d6e9078e.jpg" /></p><p>For these initial conditions, the behavior of the stochastic model closely follows that of the deterministic model (2.1) as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. Despite the value of R<sub>0</sub> being less than unity, we see that the stochastic model predicts that the disease will remain endemic in the host population. As a consequence, the behavior of the stochastic model suggests that lowering the value of R<sub>0</sub> to less than unity is no longer a sufficient condition for disease elimination.</p><p>On the other hand, the following initial conditions result in the stochastic model as well as the deterministic model (2.1) tending towards the DFE:</p><p>Initial Population:</p><p><img src="10-7401382\aa7b5602-0cd6-4b00-9893-1a105b77f990.jpg" /></p><p>In this case, both the deterministic model (2.1) and the stochastic model predict that the disease will be eliminated from the host population in time, as shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p><p>The behavior of both the stochastic and the deterministic model is therefore highly dependent on the initial conditions. We therefore conclude that due to the existence of the backward bifurcation in model (2.1), disease elimination or persistence in the region of bistability is dependent on the initial conditions of the system. If a sufficient number of infectives are present in the population, then both the stochastic as well as the deterministic model predict that there is a possibility that the disease will persist, despite R<sub>0</sub> being less than unity. Figures 3 and 4 display the forces of infection for the two different initial conditions.</p></sec><sec id="s5"><title>5. Uncertainty Analysis of R<sub>0</sub> and R<sub>c</sub></title><p>The values of R<sub>0</sub> and R<sub>c</sub> depend on the variables<img src="10-7401382\914a6444-081f-4690-9b40-60c662ab8abd.jpg" />, <img src="10-7401382\0004524b-a171-4296-ba4e-2f93a2263b8f.jpg" />and<img src="10-7401382\2a007f73-2128-4e92-9bfc-61f38c936d2b.jpg" />. While, deterministic models implicitly assume that the model parameters are not stochastic in nature, an element of uncertainty is always associated with estimates of these parameters due to factors such as natural variation, errors in measurements and lack of measuring techniques. In general, uncertainty analysis quantifies the degree of confidence in the parameter estimates by producing 95% confidence intervals (CI) which can be interpreted as intervals containing 95% of future estimates when the same assumptions are made and the only source of noise is observation error. This enables us to estimate the probability of<img src="10-7401382\d5377d5d-5555-46eb-8aea-2aaebc2baf0c.jpg" />, while taking into account the uncertainty associated with estimates of the model parameters. Our purpose in this section is to estimate the likelihood of a backward bifurcation in model (2.1) for our chosen parameter values.</p><p>We use the Latin Hypercube Sampling (LHS) to quantify the uncertainty in R<sub>0</sub> and R<sub>c</sub> as a function of the 7 model parameters <img src="10-7401382\b524e887-e5cc-4aaa-a330-91ab2d597e15.jpg" /> and<img src="10-7401382\f0eabb33-fc4e-4fcb-88d2-e2b9156817b0.jpg" />.</p><p>It is assumed that the recruitment rates <img src="10-7401382\a3117d3c-5121-445d-84b3-0445e0ba2f52.jpg" /> and <img src="10-7401382\986b228c-12a4-4029-954f-011250217d6e.jpg" /> are constants. The assumed distributions of the model parameters used in the two analyses are mentioned in <xref ref-type="table" rid="table1">Table 1</xref>. The symbols <img src="10-7401382\5c22427f-3944-43ea-9152-9c3462b15f26.jpg" /> and <img src="10-7401382\026fdc08-f98b-4537-8eb5-6094e45eb736.jpg" /> stand for the normal and gamma distributions respectively. <xref ref-type="fig" rid="fig5">Figure 5</xref> displays the assumed distributions of each of the seven model parameters along with the resultant distribution of<img src="10-7401382\07f7cce9-fc1a-40d0-a08d-85b81c9d9160.jpg" />. The probability that <img src="10-7401382\73ab839c-0733-44f2-b9d1-0b6e5a0a620c.jpg" /> for the given parameter values and distributions is 15%. Thus, for the assumed parameter values, there is a non-trivial possibility of a backward bifurcation in the model (2.1).</p></sec><sec id="s6"><title>6. Discussion</title><p>We formulate a stochastic model, based on an existing deterministic ODE model, for the transmission dynamics of dengue virus using a continuous time Markov chain. The deterministic model is known to undergo a backward bifurcation for certain values of the model parameters and consequently presents the possibility of the co-existence of both a locally asymptotically stable DFE along with a locally asymptotically stable endemic equilibrium for certain values of the basic reproduction number less than unity. It is important to note that the deterministic model (2.1) undergoes a backward bifurcation as a consequence of both the use of standard incidence, as opposed to mass action, as well as inclusion of the vector dynamics. Thus, removing the vector dynamics from model (2.1) and using a direct transmission model as suggested in [<xref ref-type="bibr" rid="scirp.30436-ref13">13</xref>], or using a mass action model [<xref ref-type="bibr" rid="scirp.30436-ref11">11</xref>] will eliminate the phenomenon of the backward bifurcation.</p><p>The numerical mean of each discrete random variable is calculated using Monte Carlo simulations. It is found that the numerically calculated means are in excellent agreement with the corresponding results from the deterministic case for parameter values, which result in the backward bifurcation. Therefore, both the stochastic model as well as the deterministic model in [<xref ref-type="bibr" rid="scirp.30436-ref11">11</xref>] predict the co-existence of a locally asymptotically stable disease-free equilibrium along with an endemic equilibrium for certain values of<img src="10-7401382\c779ab94-628e-4215-968d-8b745144254e.jpg" />. As a consequence, the stochastic model indicates that the disease may persist in the population even if<img src="10-7401382\62c185f6-12b2-4c2e-8889-6f3c1ac54db2.jpg" />.</p><p><xref ref-type="table" rid="table1">Table 1</xref>. Model parameters along with assumed values and distributions.</p><p>Parameter</p><p>Mean, variance (dist)</p><p><img src="10-7401382\25c0676f-b2e2-4ccc-8555-87123b7f73bd.jpg" /></p><p><img src="10-7401382\99278027-1b84-4920-ae1e-a1e6a264d5ad.jpg" /></p><p><img src="10-7401382\5943279d-de12-46e7-9710-4b4f0310f665.jpg" /></p><p><img src="10-7401382\1a2f1712-33fc-4d4e-8408-a45e243c4fdf.jpg" /></p><p><img src="10-7401382\2f0a0857-25ea-4779-9aca-73d7e1bee05f.jpg" /></p><p><img src="10-7401382\c7edcfc4-a25a-41fa-bd8b-d2d885369721.jpg" /></p><p><img src="10-7401382\5456c484-c0ba-4f22-b741-d3d07c107f95.jpg" /></p><p><img src="10-7401382\48aecfff-9a57-4d57-8071-a2ed37e55f6e.jpg" /></p><p><img src="10-7401382\1e20e7de-822e-4433-bb93-3c903dd155b3.jpg" /></p><p><img src="10-7401382\01dcf848-69c9-4550-bbd5-0aa9bf8aba40.jpg" /></p><p><img src="10-7401382\be2a35e7-b767-48e6-a49b-ea7e53a7f881.jpg" /></p><p><img src="10-7401382\53b0fa1f-ebd6-4cae-96e2-01589a3875ce.jpg" /></p><p><img src="10-7401382\3d78aeb3-f9f9-4009-bf9b-da91f80c9d9e.jpg" /></p><p><img src="10-7401382\38004d1e-4465-411f-9da5-ddbb31d30c5e.jpg" /></p><p><img src="10-7401382\05ef9af5-0e22-40a5-afb3-69172e8f2601.jpg" /></p><p><img src="10-7401382\41d88a1c-b4f7-4df5-bd9a-0dea1aba8ada.jpg" /></p><p>The current study focuses on a model for the spread of single strain dengue virus. However, as demonstrated by Garba et al. in [<xref ref-type="bibr" rid="scirp.30436-ref12">12</xref>], a model for the transmission dynamics of two strains of dengue with temporary cross immunity and ADE, also allows for the possibility of backward bifurcations. One possible extension of the current study therefore, is to formulate an analogous stochastic model corresponding to the deterministic model presented in [<xref ref-type="bibr" rid="scirp.30436-ref12">12</xref>] and explore the dynamics of the stochastic model for values of the model parameters which produce the bifurcation.</p></sec><sec id="s7"><title>REFERENCES</title></sec><sec id="s8"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.30436-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">S. Ranjit and N. Kissoon, “Dengue Hemorrhagic Fever and Shock Syndromes,” Pediatric Critical Care Medicine, Vol. 12, No. 1, 2011, pp. 90-100.  
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