<?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.2019.103007</article-id><article-id pub-id-type="publisher-id">AM-91282</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>
 
 
  Steady-State Analysis of SECIR Rumor Spreading Model in Complex Networks
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yujiang</surname><given-names>Liu</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>Chunmei</surname><given-names>Zeng</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>Youquan</surname><given-names>Luo</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Key Laboratory of Jiangxi Province for Numerical Simulation and Emulation Techniques, Gannan Normal University, Ganzhou, China</addr-line></aff><pub-date pub-type="epub"><day>15</day><month>03</month><year>2019</year></pub-date><volume>10</volume><issue>03</issue><fpage>75</fpage><lpage>86</lpage><history><date date-type="received"><day>19,</day>	<month>February</month>	<year>2019</year></date><date date-type="rev-recd"><day>18,</day>	<month>March</month>	<year>2019</year>	</date><date date-type="accepted"><day>21,</day>	<month>March</month>	<year>2019</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>
 
 
  In this paper, the SECIR rumor spreading model is formulated and analyzed, in which the social education level and the counterattack mechanism are taken into consideration. The results show that improving education level and increasing the ratio of counter are effective in reducing the risk of rumor propagation and enhanc
  ing
   the resistance to rumor propagation.
 
</p></abstract><kwd-group><kwd>SECIR Model</kwd><kwd> Rumor Spreading</kwd><kwd> Homogeneous Network</kwd><kwd> Counterattack Mechanism</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Rumor is a kind of social phenomenon that an unverified account or explanation of events spreads on a large-scale in a short time through people’s communication [<xref ref-type="bibr" rid="scirp.91282-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.91282-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.91282-ref3">3</xref>] . The spread of rumor can manipulate the public opinion in a locality, even can cause panic in some of the important public event [<xref ref-type="bibr" rid="scirp.91282-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.91282-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.91282-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.91282-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.91282-ref8">8</xref>] . Today, the increasing prevalence of social networking services, rumors spread by twitters, blogs, microblogs, WeChat and so on. In the Internet, the spreading of rumor is similar to epidemic spreading, but rumor’s spreading quantitative models have been rather limited in the complex network.</p><p>The standard model of rumor spreading is the Daley-Kendal (DK) model [<xref ref-type="bibr" rid="scirp.91282-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.91282-ref10">10</xref>] . The population in a local area is grouped ignorants, spreaders and stiflers. In this model, the rumor is propagated through the pair-wise contacts between spreaders and the others in the population. Spreader attempts to “infect” the other individuals with rumor. In the contact, ignorance becomes spreader, the others of individuals become stiflers. In the Maki-Thompson (MK) model [<xref ref-type="bibr" rid="scirp.91282-ref11">11</xref>] as the DK model’s variant, the spreader becomes stifler only who is the initiating spreader. The deficiencies of the DK model are considering homogeneous topology, and the simplified topology may not adequately describe the rumor’s spreading process in the Internet [<xref ref-type="bibr" rid="scirp.91282-ref12">12</xref>] - [<xref ref-type="bibr" rid="scirp.91282-ref17">17</xref>] . Zanette [<xref ref-type="bibr" rid="scirp.91282-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.91282-ref19">19</xref>] analyzed the MK model on a small-world network. His studies show that rumor “dies” in a small scale of its origin with varying network randomness. Morno et al. [<xref ref-type="bibr" rid="scirp.91282-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.91282-ref21">21</xref>] considered a rumor spreading model on a scale-free network. The results are the uniformity of the network which has a great impact on the rumor’s spreading process. Nekovee et al. [<xref ref-type="bibr" rid="scirp.91282-ref22">22</xref>] introduced the SIR model with forgetting mechanism and derived mean-field equation that describes the dynamics of rumor spreading process. His studies show that the SIR model is suitable for chain emails and large-scale information dissemination algorithms on the Internet. Zhao et al. [<xref ref-type="bibr" rid="scirp.91282-ref23">23</xref>] [<xref ref-type="bibr" rid="scirp.91282-ref24">24</xref>] refined the SIR rumor spreading model and took into account the remembering mechanism in addition to the forgetting mechanism. Zan et al. [<xref ref-type="bibr" rid="scirp.91282-ref25">25</xref>] considered the counterattack mechanism in the SIR model and introduced two models: Susceptible-infective-counterattack-Refractory (SICR) model and adjusted-SICR model. They derived mean-field equations to describe its dynamics in homogeneous network and involve steady-state analysis. Their studies show the self-resistance characteristic of networks to a rumor. Afassinou [<xref ref-type="bibr" rid="scirp.91282-ref26">26</xref>] extended the SIR model with the forgetting mechanism and population’s education rate and introduced SEIR model. He distinguishes two types of individuals in a population: educated individuals and non-educated individuals. His results show that improving the education rate of the population catalyzes the rumor spreading termination process. In social networks, when people with a higher degree of education heard a rumor which is in serious conflict with his/her belief, he/she is easier to counterattack the rumor, and even do the best to prevent the rumor propagation.</p><p>In this paper, inspiring of Zan et al. [<xref ref-type="bibr" rid="scirp.91282-ref25">25</xref>] , we consider two influential factors in rumor spreading process: the population’s education rate and the self-resistance feature of network. Motivatedly, we extend rumor spreading model―the SECIR model.</p><p>The remaining part of the paper is organized as follows. We formulate the propagation mechanism of the SECIR model in a social network, and derive a system of nonlinear ordinary differential equations that describe dynamics of rumor spreading process in Section 2. In Section 3, we analyze the steady-state of the SECIR model. We give some of the conclusions in the last section.</p></sec><sec id="s2"><title>2. Model</title><p>We study the SECIR model in a closed homogeneously mixed population that we differentiate into five distinct classes: the rumor-mongers (spreader, S), those who are spreading the rumor, the non-educated ignorants individuals class (Ignorant, I), the people who never heard the rumor, the educated ignorants individuals class (Educatee, E), the people who never heard the rumor, but have more sophisticated behaviours with the non-educated ignorant individuals when they encountered the spreader, the counterattack class (Counter, C), those who do not agree but refute the rumor, and persuade others to agree with him (refute the rumor), and the stiflers class (Recovered, R), the ones who heard the rumor but have lost interest in disseminating it. For simplicity, we refer to the rumor spreading model as the SECIR model.</p><p>According to the MK model, we assume the rumor spreads by directed contact of the spreads with others in the population, and the contacts between rumor-mongers and the rest of the population are governed by the following dynamics (As shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>):</p><p>・ Whenever a non-educated ignorant contact a spreader, the ignorant will be a relatively large probability ( β 1 ) into the spreader, but also with a smaller probability ( α 1 ) of transition to a stifler;</p><p>・ Whenever an educated ignorant contact a spreader, the ignorant will be one of the three class: spreader or stifler analog the non-educated ignorant, and he can be evolved into counterattack, and the change probability is β 2 , α 2 and θ , respectively;</p><p>・ Whenever a spreader contact a spreader, a stifler or a counter, the spreader will be into stifler with the probability g, g and η , respectively;</p><p>Let I ( t ) , E ( t ) , C ( t ) , C ( t ) , and R ( t ) respectively represent the density of the corresponding compartment in the total population. Namely that we have I ( t ) + E ( t ) + C ( t ) + S ( t ) + R ( t ) = 1 . Note that the resistance to the rumor of the educated ignorants more than the non-educated ignorants, we assume that</p><p>β 1 &gt; β 2 ,   α 1 &gt; α 2     and     η &gt; g . (1)</p><p>In accordance with the above rules, the mean-field equations of the SECIR model can be described as follows:</p><p>d I ( t ) d t = − ( β 1 + α 1 ) k &#175; I ( t ) S ( t ) d E ( t ) d t = − ( β 2 + α 2 + θ ) k &#175; E ( t ) S ( t ) d C ( t ) d t = θ k &#175; E ( t ) S ( t ) d S ( t ) d t = β 1 k &#175; I ( t ) S ( t ) + β 2 k &#175; E ( t ) S ( t ) − g k &#175; S ( t ) ( S ( t ) + R ( t ) ) − η k &#175; S ( t ) C ( t ) d R ( t ) d t = α 1 k &#175; I ( t ) S ( t ) + α 2 k &#175; E ( t ) S ( t ) + g k &#175; S ( t ) ( S ( t ) + R ( t ) ) + η k &#175; S ( t ) C ( t ) (2)</p><p>We assume that all in the population are I or E but only one spreader at the beginning of the rumor spreading, and the ratio of E to the sum of I and E is ϵ when t = 0 . Namely, when t = 0 , the initial condition of rumor spreading is given as follows:</p><p>I ( 0 ) = N − 1 N ( 1 − ϵ ) ,   E ( 0 ) = N − 1 N ϵ ,   S ( 0 ) = 1 N ,   C ( 0 ) = 0 ,   R ( 0 ) = 0. (3)</p><p>Note that for an ignorant, he/she can be a spreader or stifler, so we have β 1 + α 1 &lt; 1 , and 1 − β 1 − α 1 is the probability that no one tells him/her the rumor. For the same reason, β 2 + α 2 + θ &lt; 1 is considered.</p></sec><sec id="s3"><title>3. Model Analysis</title><p>We then postulate that the number of individuals in the I class that have heard about the rumor is the same as the number of individuals in the E class that have heard about the rumor. This simply translates to</p><p>β 1 + α 1 = β 2 + α 2 + θ = M (4)</p><p>From the first and the second equation of (2), we have</p><p>d E ( t ) d I ( t ) = E ( t ) I ( t ) (5)</p><p>Solve the above differential equation with the initial conditions (3), we obtain</p><p>E ( t ) I ( t ) = E ( 0 ) I ( 0 ) = ϵ 1 − ϵ (6)</p><p>From the first and the third Equation (2), we obtain</p><p>d C ( t ) d t = − θ α 2 + β 2 + θ d E ( t ) d t</p><p>With the initial conditions (3), we can derive the relational expression between C ( t ) and E ( t ) by separation of variable,</p><p>C ( t ) = θ α 2 + β 2 + θ ( ϵ − E ( t ) ) (7)</p><p>From (6) and (7), we have</p><p>S ( t ) + R ( t ) = 1 − ( I ( t ) + C ( t ) + E ( t ) ) = 1 − 1 − ϵ ϵ E ( t ) − θ α 2 + β 2 + θ ( ϵ − E ( t ) ) − E ( t ) = ( 1 − θ ϵ α 2 + β 2 + θ ) − ( 1 ϵ − θ α 2 + β 2 + θ ) E ( t ) (8)</p><p>Note that τ = g ϵ + ( η − g ) θ α 2 + β 2 + θ and β = 1 − ϵ ϵ β 1 + β 2 , then we have</p><p>d S ( t ) d t = β 1 k &#175; I ( t ) S ( t ) + β 2 k &#175; E ( t ) S ( t ) − g k &#175; S ( t ) ( S ( t ) + R ( t ) ) − η k &#175; S ( t ) C ( t ) = β 1 k &#175; 1 − ϵ ϵ E ( t ) S ( t ) + β 2 k &#175; E ( t ) S ( t ) − η k &#175; S ( t ) θ α 2 + β 2 + θ ( ϵ − E ( t ) )     − g k &#175; S ( t ) ( ( 1 − θ ϵ α 2 + β 2 + θ ) − ( 1 ϵ − θ α 2 + β 2 + θ ) E ( t ) ) = ( 1 − ϵ ϵ β 1 + β 2 + g ϵ + ( η − g ) θ α 2 + β 2 + θ ) k &#175; E ( t ) S ( t ) − ( g + θ ( η − g ) ϵ α 2 + β 2 + θ ) k &#175; S ( t ) = ( β + τ ) k &#175; E ( t ) S ( t ) − ϵ τ k &#175; S ( t ) (9)</p><p>From the second equation of (2), therefore (9) becomes</p><p>d S ( t ) d t = ϵ τ E ( t ) − ( β + τ ) M d E ( t ) d t</p><p>Solving the differential equations above by the method of separation of variables, we have</p><p>S ( t ) = ϵ τ M ( ln E ( t ) − ln ϵ ) − β + τ M ( E ( t ) − ϵ ) (10)</p><p>By the second equation of (2), it is easy to see that d E ( t ) d t &lt; 0 and E ( t ) are monotonically decreasing and continuous function. Let d S ( t ) d t = 0 , we obtain E ( t ) = ϵ τ β + τ . It is easy to see that, the peak value of spreader is</p><p>S max = ϵ β M + ϵ τ M ln ( τ β + τ ) (11)</p><p>d R ( t ) d t = α 1 k &#175; I ( t ) S ( t ) + α 2 k &#175; E ( t ) S ( t ) + g k &#175; S ( t ) ( S ( t ) + R ( t ) ) + η k &#175; S ( t ) C ( t ) = α 1 k &#175; 1 − ϵ ϵ E ( t ) S ( t ) + α 2 k &#175; E ( t ) S ( t ) + η k &#175; S ( t ) θ α 2 + β 2 + θ ( ϵ − E ( t ) )     + g k &#175; S ( t ) ( ( 1 − θ ϵ α 2 + β 2 + θ ) − ( 1 ϵ − θ α 2 + β 2 + θ ) E ( t ) ) = ( 1 − ϵ ϵ α 1 + α 2 − g ϵ − ( η − g ) θ α 2 + β 2 + θ ) k &#175; E ( t ) S ( t ) + ( g + θ ( η − g ) ϵ α 2 + β 2 + θ ) k &#175; S ( t ) = ( α − τ ) k &#175; E ( t ) S ( t ) + ϵ τ k &#175; S ( t ) (12)</p><p>where α = 1 − ϵ ϵ α 1 + α 2 . From the second equation of (2), therefore (12) becomes</p><p>d R ( t ) d t = ( τ − α α 2 + β 2 + θ − ϵ τ α 2 + β 2 + θ 1 E ( t ) ) d E ( t ) d t (13)</p><p>Solving the above differential equations, we get</p><p>R ( t ) = α − τ α 2 + β 2 + θ ( ϵ − E ( t ) ) + ϵ τ α 2 + β 2 + θ ( ln ϵ − ln E ( t ) ) (14)</p><p>It is easy know that S ∞ = 0 , let t → ∞ , then (8) becomes</p><p>R ∞ = ( 1 ϵ − θ α 2 + β 2 + θ ) ( ϵ − E ∞ ) (15)</p><p>Let t → ∞ , Substituting (15) into (14), it becomes</p><p>( 1 ϵ − α − τ + θ α 2 + β 2 + θ ) ( ϵ − E ∞ ) = ϵ τ α 2 + β 2 + θ ( ln ϵ − ln E ∞ ) (16)</p><p>α + β = 1 − ϵ ϵ ( β 1 + α 1 ) + ( β 2 + α 2 ) = 1 − ϵ ϵ ( β 2 + α 2 ) + ( β 2 + α 2 ) = 1 ϵ ( β 2 + α 2 + θ ) − θ (17)</p><p>Solve from (17), we get ϵ = β 2 + α 2 + θ β + α + θ , substitute into (16), we have</p><p>( ϵ − E ∞ ) = ϵ τ β + τ ( ln ϵ − ln E ∞ ) (18)</p><p>Let A ( t ) = I ( t ) + E ( t ) = 1 − ϵ ϵ E ( t ) + E ( t ) = E ( t ) / ϵ , from (18) we get the final size</p><p>A ∞ = τ β + τ ln A ∞ + 1 (19)</p><p>Theorem 1. For 0 &lt; σ &lt; 1 , the equation x = σ ln x + 1 has two solutions, x = 1 and a nontrivial solution x 1 , where 0 &lt; x 1 &lt; σ .</p><p>Proof. Obviously x = 1 is a solution of x = σ ln x + 1 .</p><p>Let f ( x ) = x − σ ln x − 1 , and take the derivative of f ( x ) with respect to x: f ′ ( x ) = 1 − σ / x , f ″ ( x ) = σ / x 2 &gt; 0 .</p><p>Let f ′ ( x ) = 0 , we obtain the unique minimum point x = σ , and the function f ( x ) is a convex function, we have f ( σ ) = σ − σ ln σ − 1 &lt; σ + σ ( 1 / σ − 1 ) − 1 = 0 , and f ( 0 + ) = ∞ . According to the Mean Value Theorem, f ( x ) have a nontrivial solution x 1 , where 0 &lt; x 1 &lt; σ . ,</p><p>Theorem 2. If the parameters are satisfied (1), (3) and (4), we have</p><p>(1) S max is decrease with ϵ , if the other parameters keep constant.</p><p>(2) S max is increase with β 1 , β 2 but decrease with α 1 , α 2 , if the other parameters keep constant.</p><p>(3) S max is decrease with g , η , if the other parameters keep constant.</p><p>Proof. (1) From (11), differential with ϵ , we have</p><p>d S max d ϵ = − β 1 − β 2 M + ϵ τ M ( ln τ β + τ ) ϵ + ( ϵ τ ) ′ ϵ M ln τ β + τ = − β 1 − β 2 M + ϵ τ M ( − β g + τ β 1 M ϵ ( β + τ ) ) + ( η − g ) θ M 2 ln τ β + τ</p><p>≤ − β 1 − β 2 M + ϵ τ M ( − β g + τ β 1 M ϵ ( β + τ ) ) + ( η − g ) θ M 2 ( τ β + τ − 1 ) = − ( ( 1 − ϵ ) β 1 + β 2 ϵ ) ( β 1 − β 2 ) M ( β + τ ) ϵ (20)</p><p>Therefore, d S max d ϵ &lt; 0 , which implies that S max decreases as ϵ increases.</p><p>(2) Since that τ = g ϵ + ( η − g ) θ α 2 + β 2 + θ and β = 1 − ϵ ϵ β 1 + β 2 , we have τ ′ β i = 0 , τ ′ α i = 0 , i = 1 , 2 , β ′ β i &gt; 0 , β ′ α i &lt; 0 . Taking the derivative of (11), with respect to β i , we have d S max d β i = ϵ M β ′ β i − ϵ τ M β ′ β i β + τ = ϵ M β β + ϵ β ′ β i &gt; 0 . It is easy to see that S max increases as β i ( i = 1 , 2 ) increases.</p><p>By the same way, we can proof that S max is decrease with α 1 , α 2 .</p><p>(3) Similarly (2), we have β ′ η = 0 , β ′ g = 0 , τ ′ x &gt; 0 , ( x = η   or   g ) , then</p><p>d S max d x = ϵ M ln τ β + τ τ ′ x + ϵ τ M ( τ ′ x τ − τ ′ x β + τ ) = ( ϵ M ln τ β + τ + ϵ β M ( β + τ ) ) τ ′ x &lt; ( ϵ M ( τ β + τ − 1 ) + ϵ β M ( β + τ ) ) τ ′ x = 0 (21)</p><p>which means that S max is decrease with g , η The proof is complete. ,</p><p>Theorem 3. If the parameters are satisfied (1), (3) and (4), we have</p><p>(1) the other parameters keep constant, the final state A ∞ is increased with ϵ .</p><p>(2) the other parameters keep constant, the final state A ∞ is decreased with β 1 , β 2 but decrease with α 1 , α 2 .</p><p>(3) the other parameters keep constant, the final state A ∞ is increased with g , η .</p><p>Proof. Let σ = τ β + τ , from (19) we have</p><p>d A ∞ d χ = d σ d χ ln A ∞ + σ 1 A ∞ d A ∞ d χ = A ∞ ln A ∞ A ∞ − σ d σ d χ (22)</p><p>From Theorem 1, 0 &lt; A ∞ &lt; σ , it is obviously that A ∞ ln A ∞ A ∞ − σ &gt; 0 , so, if we know that the plus-minus sign of d σ d χ , then the plus-minus sign of d A ∞ d χ can be determined, and furthermore, the monotonicity between A ∞ and parameters χ can be proved.</p><p>(1)</p><p>d σ d ϵ = τ ′ ϵ β − τ β ′ ϵ ( β + τ ) 2 = β 1 τ − g β ϵ 2 ( β + τ ) 2 = ( β 1 − β 2 ) g + ( η − g ) θ M β 1 ϵ 2 ( β + τ ) 2 (23)</p><p>so d σ d ϵ &gt; 0 , that is, σ increases as ϵ increases, and also implies that A ∞ increases as ϵ increases.</p><p>(2)</p><p>d σ d β i = − τ β ′ β i ( β + τ ) 2 &lt; 0 ,   ( i = 1 , 2 ) (24)</p><p>similarly, we can get d σ d α i &gt; 0 . and so A ∞ d β i &lt; 0 , A ∞ d α i &lt; 0 , where i = 1 , 2 , which proves (2).</p><p>(3)</p><p>d σ d x = τ ′ x β ( β + τ ) 2 ,   x ∈ { η , g } (25)</p><p>then, d σ d x &gt; 0 , it means that A ∞ increases as η ( g ) increases. The proof is complete.</p></sec><sec id="s4"><title>4. Numerical Simulation</title><p>We assume N = 10 5 , the average degree of network k &#175; = 10 , and the initial condition of the model follows equation of (2).</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> shows the general trends of the five kinds of agents in the SEICR rumor spreading model. We see the density of spreaders begin to expand rapidly from the initial rumor spread. As the rumor spread further, the density of spreaders reaches a peak and thereafter declines. Finally the density of spreaders is to zero and this leads to the termination of rumor spreading. And over the course of the rumor spreading, the density of ignorants and educatees always decreases, and finally evolves to zero. but the density of counter and the recovered</p><p>always decreases, and eventually evolve to a stable value.</p><p>Figures 3-5 show how the densities of spreaders change over time for different system parameters include ϵ , α 1 , β 1 , α 2 , β 2 , g and η , and the change is consistent with theorem 2. It is interest that the higher parameter β 1 , β 2 , the earlier the outbreak, the larger the peak of the outbreak, but the shorter the outbreak period (<xref ref-type="fig" rid="fig4">Figure 4</xref>). However, if the parameter X is lowered, the outbreak period will not come earlier, and the outbreak period will be longer (in <xref ref-type="fig" rid="fig5">Figure 5</xref>).</p></sec><sec id="s5"><title>5. Conclusion</title><p>In this paper, considering the social education level and the counterattack mechanism,</p><p>we analyze the dynamics of rumor propagation. The results of simulations show that improving education level and increasing the ratio of counter are effective in reducing the risk of rumor propagation and enhancing the resistance to rumor propagation.</p></sec><sec id="s6"><title>Acknowledgements</title><p>The research has been supported by The National Natural Science Foundation of China (11561004) and The 12th Five-year Education Scientific Planning Project of Jiangxi Province (15ZD3LYB031).</p></sec><sec id="s7"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s8"><title>Cite this paper</title><p>Liu, Y.J., Zeng, C.M. and Luo, Y.Q. (2019) Steady-State Analysis of SECIR Rumor Spreading Model in Complex Networks. Applied Mathematics, 10, 75-86. https://doi.org/10.4236/am.2019.103007</p></sec></body><back><ref-list><title>References</title><ref id="scirp.91282-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Peterson, W.A. and Gist, N.P. (1951) Rumor and Public Opinion. American Journal of Sociology, 57, 159-167. &lt;/br&gt;https://doi.org/10.1086/220916</mixed-citation></ref><ref id="scirp.91282-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Kesten, H. and Sidoravicius, V. (2005) The Spread of a Rumor or Infection in a Moving Population. Annals of Probability, 33, 2402-2462.  
&lt;/br&gt;https://doi.org/10.1214/009117905000000413</mixed-citation></ref><ref id="scirp.91282-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Kostka, J., Oswald, Y.A. and Wattenhofer, R. (2008) Word of Mouth: Rumor Dissemination in Social Networks. International Colloquium on Structural Information &amp; Communication Complexity, Villars-sur-Ollon, 17-20 June 2008, 185-196.  
&lt;/br&gt;https://doi.org/10.1007/978-3-540-69355-0_16</mixed-citation></ref><ref id="scirp.91282-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Ganesh, A.J., Kermarrec, A.M. and Massoulie, L. (2002) Hiscamp: Self-Organizing Hierarchical Membership Protocol. Workshop on ACM Sigops European Workshop. &lt;/br&gt;https://doi.org/10.1145/1133373.1133398</mixed-citation></ref><ref id="scirp.91282-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Thomas, S.A. (2007) Lies, Damn Lies, and Rumors: An Analysis of Collective Efficacy, Rumors, and Fear in the Wake of Katrina. Sociological Spectrum, 27, 679-703.  
&lt;/br&gt;https://doi.org/10.1080/02732170701534200</mixed-citation></ref><ref id="scirp.91282-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Bhavnani, R. and Kuklinski, J.H. (2009) Rumor Dynamics in Ethnic Violence. Journal of Politics, 71, 876. &lt;/br&gt;https://doi.org/10.1017/S002238160909077X</mixed-citation></ref><ref id="scirp.91282-ref7"><label>7</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Galam</surname><given-names> S. </given-names></name>,<etal>et al</etal>. (<year>2002</year>)<article-title>Modelling Rumors: The No Plane Pentagon French Hoax Case</article-title><source> Physica A: Statistical Mechanics &amp; Its Applications</source><volume> 320</volume>,<fpage> 571</fpage>-<lpage>580</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.91282-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Kimmel, A.J. (2004) Rumors and Rumor Control: A Manager’s Guide to Understanding and Combatting Rumors. Lawrence Erlbaum Associates.</mixed-citation></ref><ref id="scirp.91282-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Daley, D.J. and Kendall, D.G. (1965) Stochastic Rumours. IMA Journal of Applied Mathematics, 1, 42-55. &lt;/br&gt;https://doi.org/10.1093/imamat/1.1.42</mixed-citation></ref><ref id="scirp.91282-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">Daley, D.J. and Gani, J. (1999) Epidemic Modelling: An Introduction. Cambridge University Press, Cambridge. &lt;/br&gt;https://doi.org/10.1017/CBO9780511608834</mixed-citation></ref><ref id="scirp.91282-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">Maki, D.P. and Thompson, M. (1973) Mathematical Models and Applications: With Emphasis on the Social, Life, and Management Sciences. Prentice Hall, Upper Saddle River.</mixed-citation></ref><ref id="scirp.91282-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">Pittel, B. (1990) On a Daley-Kendall Model of Random Rumours. Journal of Applied Probability, 27, 14-27. &lt;/br&gt;https://doi.org/10.2307/3214592</mixed-citation></ref><ref id="scirp.91282-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">Newman, M.E., Forrest, S. and Balthrop, J. (2002) Email Networks and the Spread of Computer Viruses. Physical Review E, Statistical, Nonlinear, and Soft Matter Physics, 66, Article ID: 035101. &lt;/br&gt;https://doi.org/10.1103/PhysRevE.66.035101</mixed-citation></ref><ref id="scirp.91282-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Sudbury, A. (1985) The Proportion of the Population Never Hearing a Rumour. Journal of Applied Probability, 22, 443-446. &lt;/br&gt;https://doi.org/10.2307/3213787</mixed-citation></ref><ref id="scirp.91282-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">Holger, E., Lutz-Ingo, M. and Stefan, B. (2002) Scale-Free Topology of E-Mail Networks. Physical Review E, Statistical, Nonlinear, and Soft Matter Physics, 66, Article ID: 035103.</mixed-citation></ref><ref id="scirp.91282-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">Smith, R.D. (2002) Instant Messaging as a Scale-Free Network.</mixed-citation></ref><ref id="scirp.91282-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">Fang, W., Yamir, M. and Yaoru, S. (2006) Structure of Peer-to-Peer Social Networks. Physical Review E Statistical Nonlinear &amp; Soft Matter Physics, 73, Article ID: 036123.</mixed-citation></ref><ref id="scirp.91282-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">Zanette, D.H. (2001) Critical Behavior of Propagation on Small-World Networks. Physical Review E Statistical Nonlinear &amp; Soft Matter Physics, 64, Article ID: 050901. &lt;/br&gt;https://doi.org/10.1103/PhysRevE.64.050901</mixed-citation></ref><ref id="scirp.91282-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">Zanette, D.H. (2002) Dynamics of Rumor Propagation on Small-World Networks. Physical Review E Statistical Nonlinear &amp; Soft Matter Physics, 65, Article ID: 041908. &lt;/br&gt;https://doi.org/10.1103/PhysRevE.65.041908</mixed-citation></ref><ref id="scirp.91282-ref20"><label>20</label><mixed-citation publication-type="other" xlink:type="simple">Yamir, M., Maziar, N. and Alessandro, V. (2004) Efficiency and Reliability of Epidemic Data Dissemination in Complex Networks. Physical Review E Statistical Nonlinear &amp; Soft Matter Physics, 69, Article ID: 055101.</mixed-citation></ref><ref id="scirp.91282-ref21"><label>21</label><mixed-citation publication-type="other" xlink:type="simple">Moreno, Y., Pastorsatorras, R. and Vespignani, R. (2001) Epidemic Outbreaks in Complex Heterogeneous Networks. The European Physical Journal B Condensed Matter and Complex Systems, 26, 521-529. &lt;/br&gt;https://doi.org/10.1140/epjb/e20020122</mixed-citation></ref><ref id="scirp.91282-ref22"><label>22</label><mixed-citation publication-type="other" xlink:type="simple">Nekovee, M., Moreno, Y., Bianconi, G. and Marsili, M. (2008) Theory of Rumour Spreading in Complex Social Networks. Physica A Statistical Mechanics &amp; Its Applications, 374, 457-470. &lt;/br&gt;https://doi.org/10.1016/j.physa.2006.07.017</mixed-citation></ref><ref id="scirp.91282-ref23"><label>23</label><mixed-citation publication-type="other" xlink:type="simple">Zhao, L., Cui, H., Qiu, X. and Wang, X. (2013) Sir Rumor Spreading Model in the New Media Age. Physica A Statistical Mechanics &amp; Its Applications, 392, 995-1003.</mixed-citation></ref><ref id="scirp.91282-ref24"><label>24</label><mixed-citation publication-type="other" xlink:type="simple">Zhao, L., Wang, J., Chen, Y., Qin, W., Cheng, J. and Cui, H. (2012) Sihr Rumor Spreading Model in Social Networks. Physica A Statistical Mechanics &amp; Its Applications, 391, 2444-2453. &lt;/br&gt;https://doi.org/10.1016/j.physa.2011.12.008</mixed-citation></ref><ref id="scirp.91282-ref25"><label>25</label><mixed-citation publication-type="other" xlink:type="simple">Zan, Y., Wu, J., Ping, L. and Yu, Q. (2014) Sicr Rumor Spreading Model in Complex Networks: Counterattack and Self-Resistance. Physica A Statistical Mechanics &amp; Its Applications, 405, 159-170. &lt;/br&gt;https://doi.org/10.1016/j.physa.2014.03.021</mixed-citation></ref><ref id="scirp.91282-ref26"><label>26</label><mixed-citation publication-type="other" xlink:type="simple">Afassinou, K. (2014) Analysis of the Impact of Education Rate on the Rumor Spreading Mechanism. Physica A Statistical Mechanics &amp; Its Applications, 414, 43-52. &lt;/br&gt;https://doi.org/10.1016/j.physa.2014.07.041</mixed-citation></ref></ref-list></back></article>