<?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">OALibJ</journal-id><journal-title-group><journal-title>Open Access Library Journal</journal-title></journal-title-group><issn pub-type="epub">2333-9705</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/oalib.1102885</article-id><article-id pub-id-type="publisher-id">OALibJ-69552</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject><subject> Business&amp;Economics</subject><subject> Chemistry&amp;Materials Science</subject><subject> Computer Science&amp;Communications</subject><subject> Earth&amp;Environmental Sciences</subject><subject> Engineering</subject><subject> Medicine&amp;Healthcare</subject><subject> Physics&amp;Mathematics</subject><subject> Social Sciences&amp;Humanities</subject></subj-group></article-categories><title-group><article-title>
 
 
  Rumor Spreading of a SICS Model on Complex Social Networks with Counter Mechanism
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Chen</surname><given-names>Wan</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Tao</surname><given-names>Li</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>Yuanmei</surname><given-names>Wang</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>Xiongding</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>School of Electronics and Information, Yangtze University, Jingzhou, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>wanchen520@126.com(CW)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>31</day><month>07</month><year>2016</year></pub-date><volume>03</volume><issue>07</issue><fpage>1</fpage><lpage>11</lpage><history><date date-type="received"><day>7</day>	<month>July</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>22</month>	<year>July</year>	</date><date date-type="accepted"><day>26</day>	<month>July</month>	<year>2016</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>
 
 
   
   The rumor spreading has been widely studied by scholars. However, there exist some people who will persuade infected individuals to resist and counterattack the rumor propagation in our social life. In this paper, a new 
   SICS
    (susceptible-infected-counter-susceptible) rumor spreading model with counter mechanism on complex social networks is presented. Using the mean-field theory the spreading dynamics of the rumor is studied in detail. We obtain the basic reproductive number 
   r
    
   and equilibriums. The basic reproductive number is correlated to the network topology and the influence of the counter mechanism. When 
   <strong style="line-height:1.5;"><em>ρ</em></strong>
   <strong style="line-height:1.5;">＜1</strong>
   , the rumor-free equilibrium is globally asymptotically stable, and when 
   <em>ρ</em>＞1
   , the positive equilibrium is permanent. Some interesting patterns of rumor spreading involved with counter force have been revealed. Finally, numerical simulations have been given to demonstrate the effectiveness of the theoretical analysis. 
  
 
</p></abstract><kwd-group><kwd>Rumor Spreading Model</kwd><kwd> Complex Social Networks</kwd><kwd> Counter Mechanism</kwd><kwd> Stability</kwd><kwd> Permanence</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Nowadays, more and more SNS (Social Networking Services) networks are emerging in our social life, such as Facebook, WeChat, LinkedIn and so on, which are seemingly like cobwebs to connect people from different places. With the rapid increase of the number of SNS users, rumor will be quickly into people’s horizons. Each coin has its two sides, as the rumors spread on the impact of our social lives. Sometimes, the rumor spreading may play a positive role, for instance, we can let more people to concern about something and take pertinent precaution measures by utilizing the rapid and efficient characteristic of rumor spreading [<xref ref-type="bibr" rid="scirp.69552-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.69552-ref2">2</xref>] . However, most rumors induce public panic, social disarray and severe economic loss, etc. [<xref ref-type="bibr" rid="scirp.69552-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.69552-ref4">4</xref>] . Therefore, it is very important to investigate the mechanism of rumor spreading and how to effectively control the rumor.</p><p>Rumor can be viewed as an “infection of the mind”, and its spreading shows an interesting similarity to the epidemic spreading [<xref ref-type="bibr" rid="scirp.69552-ref5">5</xref>] - [<xref ref-type="bibr" rid="scirp.69552-ref9">9</xref>] . Daley and Kendal [<xref ref-type="bibr" rid="scirp.69552-ref5">5</xref>] first proposed the classic DK model of rumor spreading. Since then, most of the studies are based on DK model [<xref ref-type="bibr" rid="scirp.69552-ref10">10</xref>] - [<xref ref-type="bibr" rid="scirp.69552-ref17">17</xref>] . In order to overcome the weaknesses of DK model, more and more researchers consider the topological characteristics of underlying networks that they have started to study the problems of rumor spreading on complex networks [<xref ref-type="bibr" rid="scirp.69552-ref15">15</xref>] - [<xref ref-type="bibr" rid="scirp.69552-ref20">20</xref>] . Nekovee and Moreno et al. [<xref ref-type="bibr" rid="scirp.69552-ref16">16</xref>] derived a conclusion that scale-free social networks were prone to the spreading of rumors. In Ref. [<xref ref-type="bibr" rid="scirp.69552-ref17">17</xref>] , the authors found that the degree distribution influenced directly the final rumor size. Recently, researchers [<xref ref-type="bibr" rid="scirp.69552-ref18">18</xref>] - [<xref ref-type="bibr" rid="scirp.69552-ref20">20</xref>] started to take full into account of the role of human behaviors and different mechanisms in the rumor spreading. Zhao et al. [<xref ref-type="bibr" rid="scirp.69552-ref18">18</xref>] presented a novel model by introducing the forget mechanism. Wang et al. [<xref ref-type="bibr" rid="scirp.69552-ref19">19</xref>] presented a novel SIR model by introducing the trust mechanism between the ignorant nodes and the spreader nodes. Han et al. [<xref ref-type="bibr" rid="scirp.69552-ref20">20</xref>] presented a novel model based on the heat energy theory to analyze the mechanisms of rumor propagation on social networks.</p><p>However, most of the previous models didn’t consider that people may not agree with the rumor and counterattack it strongly. Based on some realistic perspectives, different people may have different views to the rumor on social networks. Some people may be in conflict with their beliefs when they hear rumor. They will persuade infected individuals to resist and counterattack the rumor propagation. In order to study this phenomenon, we present a SICS (susceptible-infected-counter-susceptible) rumor spreading model with counter mechanism on complex social networks to explain it. Obviously, the counter mechanism can change the contacts among people, i.e. network topology structure. Within the counter mechanism of the SICS model, when an infected individual contacts a counter individual, it may become a counter individual with a certain probability.</p><p>The rest of this paper is organized as follows. In Section 2, we present a SICS rumor spreading model and derive the corresponding mean-field equations to describe the dynamics of the model. In Section 3, the basic reproductive number obtained at first. Then we analyze the globally asymptotic stability of rumor-free equilibrium and the permanence of the rumor in detail. Simulation results of the proposed model are shown in Section 4. Finally, we conclude the paper in Section 5.</p></sec><sec id="s2"><title>2. Model Formulation</title><p>As mentioned earlier, we present a SICS rumor spreading model. The population is divided into three classes: susceptible individuals who have ambiguous attitude about the rumor; infected individuals who believe and spread it actively; counter individuals who reject the rumor, refute the rumor and persuade neighbors don’t believe in it. Taking into account the heterogeneity induced by the presence of vertices with different connectivities, let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x9.png" xlink:type="simple"/></inline-formula> be the densities of susceptible, infected and counter individuals of connectivity k at time t, respectively.</p><p>The SICS model has the flow diagram given in <xref ref-type="fig" rid="fig1">Figure 1</xref>. In the course of rumor spreading, a susceptible individual is infected with probability <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x10.png" xlink:type="simple"/></inline-formula> if it is connected to an infected individual. When a counter individual</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> The flow diagram of the SICS model</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/69552x11.png"/></fig><p>contacts an infected individual, the counter individual can persuade infected individual to resist and counterattack the rumor, so the infected individual becomes a counter node with probability<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x12.png" xlink:type="simple"/></inline-formula>. A susceptible individual transform into a counter individual with probability<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x13.png" xlink:type="simple"/></inline-formula>. Due to some own reason, an infected individual turns into a counter individual with probability<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x14.png" xlink:type="simple"/></inline-formula>. However, some counter individuals, due to loss of counterattack ability, join the susceptible individuals again, i.e., moving back to susceptible state, with probability<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x15.png" xlink:type="simple"/></inline-formula>. We assume that the immigration rate and emigration rate are both constant l in the spreading process of rumor. All recruitment is into the susceptible class.</p><p>Thus, the dynamic mean-field reaction rate equations can be written as</p><disp-formula id="scirp.69552-formula480"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69552x16.png"  xlink:type="simple"/></disp-formula><p>The probability <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x17.png" xlink:type="simple"/></inline-formula> describes a link pointing to an infected individual,</p><disp-formula id="scirp.69552-formula481"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69552x18.png"  xlink:type="simple"/></disp-formula><p>the probability <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x19.png" xlink:type="simple"/></inline-formula> describes a link pointing to a counter individual which satisfies the relation</p><disp-formula id="scirp.69552-formula482"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69552x20.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x21.png" xlink:type="simple"/></inline-formula> is the average degree within the network. And <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x22.png" xlink:type="simple"/></inline-formula> is the density of infected individuals in the whole network, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x23.png" xlink:type="simple"/></inline-formula>is the density of counter individuals in the whole network, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x24.png" xlink:type="simple"/></inline-formula>is the connectivity distribution.</p></sec><sec id="s3"><title>3. Stability Analysis</title><p>In this section, we present an analytic solution to the deterministic equations describing the dynamic of the (SICS) rumor spreading process.</p><p>Theorem 1. Let.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x25.png" xlink:type="simple"/></inline-formula>. There always exists a rumor-free equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x26.png" xlink:type="simple"/></inline-formula> and when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x27.png" xlink:type="simple"/></inline-formula>, then system (1) has a positive equilibrium solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x28.png" xlink:type="simple"/></inline-formula>.</p><p>Proof. To get the equilibrium solution<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x29.png" xlink:type="simple"/></inline-formula>, we need to make the right side of system (1) equal to zero. Then the equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x30.png" xlink:type="simple"/></inline-formula> should satisfy</p><disp-formula id="scirp.69552-formula483"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69552x31.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x32.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x33.png" xlink:type="simple"/></inline-formula>, one has</p><disp-formula id="scirp.69552-formula484"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69552x34.png"  xlink:type="simple"/></disp-formula><p>According to the following normalization condition for all k:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x35.png" xlink:type="simple"/></inline-formula>.</p><p>We can obtain:</p><disp-formula id="scirp.69552-formula485"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69552x36.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.69552-formula486"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69552x37.png"  xlink:type="simple"/></disp-formula><p>Inserting Equation (6) into Equation (2), we obtain the following equation</p><disp-formula id="scirp.69552-formula487"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69552x38.png"  xlink:type="simple"/></disp-formula><p>Inserting Equation (7) into Equation (3), we obtain the following equation</p><disp-formula id="scirp.69552-formula488"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69552x39.png"  xlink:type="simple"/></disp-formula><p>Equation (9) divided by Equation (8), we obtain the following equation</p><disp-formula id="scirp.69552-formula489"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69552x40.png"  xlink:type="simple"/></disp-formula><p>Inserting Equation (10) into Equation (8), we can obtain</p><disp-formula id="scirp.69552-formula490"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69552x41.png"  xlink:type="simple"/></disp-formula><p>Obviously, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x42.png" xlink:type="simple"/></inline-formula>is a solution of Equation (11), i.e.,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x43.png" xlink:type="simple"/></inline-formula>. To ensure Equation (11) have a nontrivial solution, i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x44.png" xlink:type="simple"/></inline-formula>, the following conditions must be satisfied</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x45.png" xlink:type="simple"/></inline-formula>.</p><p>We can obtain the basic reproductive number</p><disp-formula id="scirp.69552-formula491"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69552x46.png"  xlink:type="simple"/></disp-formula><p>So, a nontrivial solution exists if and only if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x47.png" xlink:type="simple"/></inline-formula>.</p><p>Substitute the nontrivial solution of (11) into (6), we can get<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x48.png" xlink:type="simple"/></inline-formula>. By (5) and (6), we can easily obtain</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x49.png" xlink:type="simple"/></inline-formula>.</p><p>Therefore, the positive equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x50.png" xlink:type="simple"/></inline-formula> is well-defined. Hence, when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x51.png" xlink:type="simple"/></inline-formula>, one and only one positive equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x52.png" xlink:type="simple"/></inline-formula> of system (1) exists. This completes the proof.</p><p>Remark. The basic reproductive number is obtained by Equation (12), which depends on the fluctuations of the degree distribution and the influence of counter mechanism. The <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x53.png" xlink:type="simple"/></inline-formula> can affect the basic reproductive number.</p><p>Theorem 2. If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x54.png" xlink:type="simple"/></inline-formula>, the rumor-free equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x55.png" xlink:type="simple"/></inline-formula> of the system (1) is globally asymptotically stable.</p><p>Proof. We rewrite the system (1) as</p><disp-formula id="scirp.69552-formula492"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69552x56.png"  xlink:type="simple"/></disp-formula><p>The Jacobian matrix of system (13) at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x57.png" xlink:type="simple"/></inline-formula> is a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x58.png" xlink:type="simple"/></inline-formula> as follows</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x59.png" xlink:type="simple"/></inline-formula>,</p><p>where</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x60.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x61.png" xlink:type="simple"/></inline-formula>.</p><p>By mathematical induction method, the characteristic equation can be calculated as follows</p><disp-formula id="scirp.69552-formula493"><graphic  xlink:href="http://html.scirp.org/file/69552x62.png"  xlink:type="simple"/></disp-formula><p>where</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x63.png" xlink:type="simple"/></inline-formula>.</p><p>The stability of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x64.png" xlink:type="simple"/></inline-formula> is only dependent on</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x65.png" xlink:type="simple"/></inline-formula>.</p><p>Note that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x66.png" xlink:type="simple"/></inline-formula>.</p><p>So, we have obtained</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x67.png" xlink:type="simple"/></inline-formula>.</p><p>When<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x68.png" xlink:type="simple"/></inline-formula>, all real-valued eigenvalues are negative. Hence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x69.png" xlink:type="simple"/></inline-formula>is locally asymptotically stable if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x70.png" xlink:type="simple"/></inline-formula>.</p><p>Now we will prove that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x71.png" xlink:type="simple"/></inline-formula> is globally attractive. From the second equation of system (1) we can get</p><disp-formula id="scirp.69552-formula494"><graphic  xlink:href="http://html.scirp.org/file/69552x72.png"  xlink:type="simple"/></disp-formula><p>Now we consider the comparison equation with the condition <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x73.png" xlink:type="simple"/></inline-formula> as follows</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x74.png" xlink:type="simple"/></inline-formula>,</p><p>integrating from 0 to t yields</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x75.png" xlink:type="simple"/></inline-formula>.</p><p>Since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x76.png" xlink:type="simple"/></inline-formula>, we obtain<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x77.png" xlink:type="simple"/></inline-formula> as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x78.png" xlink:type="simple"/></inline-formula>.</p><p>According to the comparison theorem of functional differential equation, we can get<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x79.png" xlink:type="simple"/></inline-formula>, for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x80.png" xlink:type="simple"/></inline-formula>.</p><p>Thus, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x81.png" xlink:type="simple"/></inline-formula>as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x82.png" xlink:type="simple"/></inline-formula>, which implies <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x83.png" xlink:type="simple"/></inline-formula> as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x84.png" xlink:type="simple"/></inline-formula>, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x85.png" xlink:type="simple"/></inline-formula>. It follows that the rumor-free equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x86.png" xlink:type="simple"/></inline-formula> is globally attractive. This completes the proof.</p><p>Theorem 3. If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x87.png" xlink:type="simple"/></inline-formula>, the rumor is permanent on complex social networks, i.e., there exists a<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x88.png" xlink:type="simple"/></inline-formula>, such that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x89.png" xlink:type="simple"/></inline-formula>.</p><p>Proof. We will use the result of Thieme in Theorem 4.6 [<xref ref-type="bibr" rid="scirp.69552-ref21">21</xref>] to prove it. Define</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x90.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x91.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x92.png" xlink:type="simple"/></inline-formula>.</p><p>In the following, we will show that (1) is uniformly persistent with respect to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x93.png" xlink:type="simple"/></inline-formula>.</p><p>Obviously, X is positively invariant with respect to system (1). If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x94.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x95.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x96.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x97.png" xlink:type="simple"/></inline-formula>, then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x98.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x99.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x100.png" xlink:type="simple"/></inline-formula> for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x101.png" xlink:type="simple"/></inline-formula>. Since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x102.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x103.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x104.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x105.png" xlink:type="simple"/></inline-formula>, we have<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x106.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x107.png" xlink:type="simple"/></inline-formula>. Thus, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x108.png" xlink:type="simple"/></inline-formula>is also positively invariant. Furthermore, there exists a compact set B in which all solutions of (1) initiated in X will enter and remain forever after. The compactness condition (C4.2) in Thieme [<xref ref-type="bibr" rid="scirp.69552-ref21">21</xref>] is easily verified for this set B. Denote</p><disp-formula id="scirp.69552-formula495"><graphic  xlink:href="http://html.scirp.org/file/69552x109.png"  xlink:type="simple"/></disp-formula><p>Denote</p><disp-formula id="scirp.69552-formula496"><graphic  xlink:href="http://html.scirp.org/file/69552x110.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x111.png" xlink:type="simple"/></inline-formula> is the omega limit set of the solutions of system (1) starting in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x112.png" xlink:type="simple"/></inline-formula>. Restricting system (1) on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x113.png" xlink:type="simple"/></inline-formula> gives</p><disp-formula id="scirp.69552-formula497"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/69552x114.png"  xlink:type="simple"/></disp-formula><p>It is easy to verify that system (13) has a unique equilibrium <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x115.png" xlink:type="simple"/></inline-formula> in X. Thus <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x116.png" xlink:type="simple"/></inline-formula> is the unique equilibrium of system (1) in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x117.png" xlink:type="simple"/></inline-formula>. It is easy to check that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x118.png" xlink:type="simple"/></inline-formula> is locally asymptotically stable. This implies that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x119.png" xlink:type="simple"/></inline-formula> is globally asymptotically stable for (13) is a linear system. Therefore<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x120.png" xlink:type="simple"/></inline-formula>. And <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x121.png" xlink:type="simple"/></inline-formula><sub> </sub>is a covering of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x122.png" xlink:type="simple"/></inline-formula>, which is isolated and is acyclic (since there exists no solution in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x123.png" xlink:type="simple"/></inline-formula> which links <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x124.png" xlink:type="simple"/></inline-formula> to itself). Finally, the proof will be done if we show <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x125.png" xlink:type="simple"/></inline-formula> is a weak repeller for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x126.png" xlink:type="simple"/></inline-formula>, i.e.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x127.png" xlink:type="simple"/></inline-formula>,</p><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x128.png" xlink:type="simple"/></inline-formula> is an arbitrarily solution with initial value in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x129.png" xlink:type="simple"/></inline-formula>. By Leenheer and Smith (2003, Proof of Lemma 3.5, [<xref ref-type="bibr" rid="scirp.69552-ref22">22</xref>] ), we need only to prove <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x130.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x131.png" xlink:type="simple"/></inline-formula> is the stable manifold of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x132.png" xlink:type="simple"/></inline-formula>. Suppose it is not true, then there exists a solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x133.png" xlink:type="simple"/></inline-formula> in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x131.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x134.png" xlink:type="simple"/></inline-formula>, such that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x135.png" xlink:type="simple"/></inline-formula>as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x136.png" xlink:type="simple"/></inline-formula>. (15)</p><p>Since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x137.png" xlink:type="simple"/></inline-formula>, we can choose <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x137.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x138.png" xlink:type="simple"/></inline-formula> such that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x139.png" xlink:type="simple"/></inline-formula>.</p><p>For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x140.png" xlink:type="simple"/></inline-formula>, by (15) there exists a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x141.png" xlink:type="simple"/></inline-formula> such that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x142.png" xlink:type="simple"/></inline-formula>.</p><p>For all <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x143.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x144.png" xlink:type="simple"/></inline-formula>. Let</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x145.png" xlink:type="simple"/></inline-formula>.</p><p>The derivative of V along the solution is given by</p><disp-formula id="scirp.69552-formula498"><graphic  xlink:href="http://html.scirp.org/file/69552x146.png"  xlink:type="simple"/></disp-formula><p>Hence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x147.png" xlink:type="simple"/></inline-formula> as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x148.png" xlink:type="simple"/></inline-formula>, which contradicts to the boundedness of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x149.png" xlink:type="simple"/></inline-formula>. This completes the proof.</p></sec><sec id="s4"><title>4. Numerical Simulations</title><p>In this section, several numerical simulations are presented to illustrate our analysis. We consider the system (1) on a complex social network with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x150.png" xlink:type="simple"/></inline-formula>, where the parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x151.png" xlink:type="simple"/></inline-formula> satisfies<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x152.png" xlink:type="simple"/></inline-formula>.</p><p>In <xref ref-type="fig" rid="fig2">Figure 2</xref>, the parameters are chosen as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x153.png" xlink:type="simple"/></inline-formula> then the basic reproductive number<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x154.png" xlink:type="simple"/></inline-formula>. We can see that when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x155.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x156.png" xlink:type="simple"/></inline-formula>grows to zero, i.e., the infectious individuals will ultimately disappear.</p><p>In <xref ref-type="fig" rid="fig3">Figure 3</xref>, we choose <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x157.png" xlink:type="simple"/></inline-formula> thus the basic reproductive number<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x158.png" xlink:type="simple"/></inline-formula>. We can see that when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x159.png" xlink:type="simple"/></inline-formula>, the rumor is persist and the infected individuals’ number will converge to a positive constant respectively.</p><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> The time series of system (1) with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x161.png" xlink:type="simple"/></inline-formula> and initial values<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x162.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x163.png" xlink:type="simple"/></inline-formula></title></caption><fig id ="fig2_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/69552x160.png"/></fig></fig-group><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> The time series of system (1) with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x165.png" xlink:type="simple"/></inline-formula> and initial values<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x166.png" xlink:type="simple"/></inline-formula>,<img data-original="http://html.scirp.org/file/69552x167.png" /></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/69552x164.png"/></fig><p>In <xref ref-type="fig" rid="fig4">Figure 4</xref>, numerical simulations show the spread of SICS model on complex social networks with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x168.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x169.png" xlink:type="simple"/></inline-formula>. The condition of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x170.png" xlink:type="simple"/></inline-formula>, that different <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x171.png" xlink:type="simple"/></inline-formula> leading to different states. In addition, it is also found that the larger the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x168.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x172.png" xlink:type="simple"/></inline-formula> is, the rumor dies out faster.</p><p>In <xref ref-type="fig" rid="fig5">Figure 5</xref>, numerical simulations show the spread of SICS model on complex social networks with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x173.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x174.png" xlink:type="simple"/></inline-formula>. The condition of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x175.png" xlink:type="simple"/></inline-formula>, that different <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x176.png" xlink:type="simple"/></inline-formula> leading to different states. In addition, it is also found that the larger the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x173.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x177.png" xlink:type="simple"/></inline-formula> is, the positive equilibrium will be lower. The simulations indicate that the numerical results are well consistent with the theoretical analysis.</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> The prevalence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x179.png" xlink:type="simple"/></inline-formula> versus t corresponding to different <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x180.png" xlink:type="simple"/></inline-formula> with identical initial value<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x181.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/69552x178.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> The prevalence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x183.png" xlink:type="simple"/></inline-formula> versus t corresponding to different <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x184.png" xlink:type="simple"/></inline-formula> with identical initial value<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x184.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x185.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/69552x182.png"/></fig></sec><sec id="s5"><title>5. Conclusion</title><p>In summary, we present a new SICS rumor spreading model with counter mechanism on complex social networks. By using the mean-field theory, we obtain the basic reproductive number and equilibriums. Theoretical results indicate that the basic reproductive number is significantly dependent on the topology of the underlying networks and the counter mechanism. The basic reproductive number is in direct proportion to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x186.png" xlink:type="simple"/></inline-formula>. So, network heterogeneity makes rumor easy to spread. Moreover, we found that the greater <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x187.png" xlink:type="simple"/></inline-formula> can decrease the basic reproductive number<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/69552x188.png" xlink:type="simple"/></inline-formula>, i.e., lower average rumor density and shorter rumor prevalent decay time. The global stability of rumor-free equilibrium and the permanence of rumor are proved in detail. Our theoretical and numerical simulation results give a novel explanation for rumor spreading. This study has valuable guiding significance in effectively preventing rumor spreading.</p></sec><sec id="s6"><title>Acknowledgements</title><p>This work was supported in part by the National Natural Science Foundation of China under Grant 60973012.</p></sec><sec id="s7"><title>Cite this paper</title><p>Chen Wan,Tao Li,Yuanmei Wang,Xiongding Liu, (2016) Rumor Spreading of a SICS Model on Complex Social Networks with Counter Mechanism. Open Access Library Journal,03,1-11. doi: 10.4236/oalib.1102885</p></sec><sec id="s8"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.69552-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Galam, S. (2003) Modelling Rumors: The No Plane Pentagon French Hoax Case. 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