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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Phys.</journal-id>
<journal-title>Frontiers in Physics</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Phys.</abbrev-journal-title>
<issn pub-type="epub">2296-424X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="publisher-id">1213044</article-id>
<article-id pub-id-type="doi">10.3389/fphy.2023.1213044</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Physics</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Exploring the formation dynamics of affective polarization by considering coupled feedback</article-title>
<alt-title alt-title-type="left-running-head">Cui</alt-title>
<alt-title alt-title-type="right-running-head">
<ext-link ext-link-type="uri" xlink:href="https://doi.org/10.3389/fphy.2023.1213044">10.3389/fphy.2023.1213044</ext-link>
</alt-title>
</title-group>
<contrib-group>
<contrib contrib-type="author" corresp="yes">
<name>
<surname>Cui</surname>
<given-names>Peng-Bi</given-names>
</name>
<xref ref-type="corresp" rid="c001">&#x2a;</xref>
<uri xlink:href="https://loop.frontiersin.org/people/1731862/overview"/>
</contrib>
</contrib-group>
<aff>
<institution>International Academic Center of Complex Systems</institution>, Beijing Normal University, <addr-line>Zhuhai</addr-line>, <country>China</country>
</aff>
<author-notes>
<fn fn-type="edited-by">
<p>
<bold>Edited by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1048269/overview">Xiaoke Xu</ext-link>, Dalian Nationalities University, China</p>
</fn>
<fn fn-type="edited-by">
<p>
<bold>Reviewed by:</bold> <ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1277122/overview">Zhidan Zhao</ext-link>, Shantou University, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/2304488/overview">Shimin Cai</ext-link>, University of Electronic Science and Technology Hospital, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/2304627/overview">Paolo Pin</ext-link>, University of Siena, Italy</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/2308439/overview">Xiaolong Chen</ext-link>, Southwestern University of Finance and Economics, China</p>
<p>
<ext-link ext-link-type="uri" xlink:href="https://loop.frontiersin.org/people/1515662/overview">Zhixi Wu</ext-link>, Lanzhou University, China</p>
</fn>
<corresp id="c001">&#x2a;Correspondence: Peng-Bi Cui, <email>cuisir610@gmail.com</email>
</corresp>
</author-notes>
<pub-date pub-type="epub">
<day>16</day>
<month>06</month>
<year>2023</year>
</pub-date>
<pub-date pub-type="collection">
<year>2023</year>
</pub-date>
<volume>11</volume>
<elocation-id>1213044</elocation-id>
<history>
<date date-type="received">
<day>27</day>
<month>04</month>
<year>2023</year>
</date>
<date date-type="accepted">
<day>30</day>
<month>05</month>
<year>2023</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#xa9; 2023 Cui.</copyright-statement>
<copyright-year>2023</copyright-year>
<copyright-holder>Cui</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/">
<p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p>
</license>
</permissions>
<abstract>
<p>Polarization issues are generally subject to ideological and affective polarization. Particularly, affective polarization generally accelerates the polarization process. Yet, a wide array of the existing literature has not provided valid ways to make distinctions between them. Therefore, the mechanism contributing to the rise of affective polarization still remains unclear, along with its unique emergent dynamics. To address this issue, we introduces the coupled feedback between opinions and response susceptibility to an attraction&#x2013;repulsion model which takes into account three parameters: interaction strength, response susceptibility, and tolerance to others. The model features phase diagrams of global consensus, affective polarization, and &#x201C;harmony with diversity&#x201d; states. Subsequently, we proceed simulations on time-varying and static social networks, showing that intermediate parameter ranges yield a global consensus as one integrated cluster collapsing and converging toward an uncertain moderate position after long-term persistence. The feedback essentially offers a counterforce to establish an inversion between the global consensus and &#x201C;harmony with diversity&#x201D;. Remarkably, strengthening feedback may facilitate polarization by driving the system to first self-organize into one integrated cluster, which then gradually approaches polarization, especially for low tolerance and strong interactions, whereby the step-like dynamic behaviors of opinion entropy suggest the occurrence of a dynamic equilibrium. In summary, the aforementioned phenomena have never been unearthed before and can be regarded as unique dynamics features of affective polarization. Finally, this study attempts to offer a useful approach to the micro foundations of affective polarization for the first time, and the results guide us on how to avoid the dilemmas of this polarization.</p>
</abstract>
<kwd-group>
<kwd>opinion dynamics</kwd>
<kwd>bounded confidence</kwd>
<kwd>social networks</kwd>
<kwd>affective polarization</kwd>
<kwd>coupled feedback</kwd>
<kwd>global consensus</kwd>
<kwd>opinion entropy</kwd>
</kwd-group>
<contract-sponsor id="cn001">National Natural Science Foundation of China<named-content content-type="fundref-id">10.13039/501100001809</named-content>
</contract-sponsor>
<custom-meta-wrap>
<custom-meta>
<meta-name>section-at-acceptance</meta-name>
<meta-value>Social Physics</meta-value>
</custom-meta>
</custom-meta-wrap>
</article-meta>
</front>
<body>
<sec id="s1">
<title>1 Introduction</title>
<p>Polarization is, here, conceived as a process of growing constraints in people&#x2019;s viewpoints and further emergence of alignments along multiple or even opposite lines of potential disagreement [<xref ref-type="bibr" rid="B1">1</xref>&#x2013;<xref ref-type="bibr" rid="B3">3</xref>]. Nowadays, the world is being perplexed by the growth of polarization [<xref ref-type="bibr" rid="B4">4</xref>,<xref ref-type="bibr" rid="B5">5</xref>]. It is, thus, increasingly a concern to understand the nature and causes of polarization and how to prevent the public from reaching dangerous degrees of polarization [<xref ref-type="bibr" rid="B6">6</xref>&#x2013;<xref ref-type="bibr" rid="B11">11</xref>].</p>
<p>There exist at least two kinds of polarization that can be easily carried to extremes and undermine the foundation of social order: ideological polarization (IP) [<xref ref-type="bibr" rid="B12">12</xref>], which indicates an opposite political view among elites, and affective polarization (AP), whereby individuals develop negative attitudes toward members of the opposing party and become entrenched [<xref ref-type="bibr" rid="B13">13</xref>&#x2013;<xref ref-type="bibr" rid="B18">18</xref>]. IP and AP have been rising during the last decade [<xref ref-type="bibr" rid="B16">16</xref>,<xref ref-type="bibr" rid="B19">19</xref>]. Furthermore, IP refers to the fact that political views are widely dispersed and heterogeneous, or bimodal, among elites. Unlike IP, which is largely driven by rational self-interest motivations [<xref ref-type="bibr" rid="B12">12</xref>,<xref ref-type="bibr" rid="B20">20</xref>&#x2013;<xref ref-type="bibr" rid="B23">23</xref>], AP itself generally suggests strong affective decision-making with a coupling relationship between individuals&#x2019; opinions and their subsequent responses [<xref ref-type="bibr" rid="B15">15</xref>]. This coupling relationship essentially creates a negative feedback mechanism, which has been widely observed in empirical cases [<xref ref-type="bibr" rid="B15">15</xref>]. For example, individuals with higher levels of out-party animosity report taking a more strong stand against those from the other party (for example, they would not even receive any suggestions from those from the other party) [<xref ref-type="bibr" rid="B12">12</xref>] and having more difficulty in repositioning, which is regardless of economic self-interest. The adverse effects of AP can spill over from the political area to other issues such as COVID-19 vaccines [<xref ref-type="bibr" rid="B24">24</xref>], gun-control [<xref ref-type="bibr" rid="B25">25</xref>], and abortion [<xref ref-type="bibr" rid="B26">26</xref>], which is much more harmful than IP. Therefore, AP might have unique dynamics, behind which the mentioned micro negative feedback can naturally be a potential responsible mechanism.</p>
<p>Up to now, a large body of existing studies has explored various mechanisms which are responsible for clustering of beliefs and polarization, especially IP, in complex social systems [<xref ref-type="bibr" rid="B2">2</xref>,<xref ref-type="bibr" rid="B9">9</xref>,<xref ref-type="bibr" rid="B20">20</xref>,<xref ref-type="bibr" rid="B27">27</xref>&#x2013;<xref ref-type="bibr" rid="B32">32</xref>], and the mutually reinforcing relation between IP and AP has also been identified. For example, Americans increasingly dislike those of the other party because of intense struggles between Democrats and Republicans [<xref ref-type="bibr" rid="B15">15</xref>,<xref ref-type="bibr" rid="B33">33</xref>,<xref ref-type="bibr" rid="B34">34</xref>], which conversely gives rise to an increasing IP among the US public, rising social inequality, and conflicts [<xref ref-type="bibr" rid="B35">35</xref>]. Furthermore, polarization among elites has become mainly affective rather than ideological. The aforementioned realistic problem suggests a call for further explorations to identify the unique dynamic features of AP so as to develop more effective preventing measures to slow or even stop the accelerating polarization process, which has nevertheless received very little attention in the growing literature. Due to the positive feedback, however, the growth of AP seems to have multiple contributing factors, including economic adversity, racial animus, cultural values, religions, gender polarization, and a range of other socioeconomic factors [<xref ref-type="bibr" rid="B34">34</xref>,<xref ref-type="bibr" rid="B36">36</xref>&#x2013;<xref ref-type="bibr" rid="B38">38</xref>], making the exploration of the unique features of AP arduous. Since the general micro foundation of AP dynamics remains unclear. It leads to the following questions to be addressed: what are the micro foundation of AP dynamics and the unique dynamic features of AP? How does the micro mechanism govern the AP dynamics, together with other potential factors such as interaction strength, response susceptibility, and tolerance level?</p>
<p>In order to address these questions arising from the lack of micro foundation in AP, we adopt a novel attraction&#x2013;repulsion model (ARM) that captures the coupled feedback between individuals&#x2019; opinions and their responses, which essentially belongs to the negative feedback class. The proposed model constructs an adaptive-system perspective on the effects of the rules on emergent dynamics of not only AP and global census (GC) but also the &#x201c;harmony with diversity&#x201d; (HD) state, which has been recently identified [<xref ref-type="bibr" rid="B39">39</xref>]. It should be noted that the opinion updating rules in our model paradigm are based on a simple assumption that an individual&#x2019;s attraction to or repulsion from others is only governed by the opinion dissimilarity between them, rather than the positions themselves. In addition, interaction strength, response susceptibility, and individual tolerance have been viewed as vital regulation factors to be considered. We are concerned with how the negative feedback mechanism governs the emergent dynamics of AP, together with the three vital regulation factors.</p>
<p>The discoveries of this study include the following: 1) the identification of conditions under which a population approaches convergence into a moderate position; 2) the identification of the conditions under which the population becomes highly polarized with asymmetric opposite camps or even extremely polarized with symmetric opposite extreme camps, and under which it enters a desired HD state with a stable integrated opinion cluster centering on a neutral point; 3) the transitions between the three states and the triple point; 4) opinions of the majority may first self-organize into one integrated cluster, which then approaches the boundary of an ideological space because of the counterforce exerted by the negative coupled feedback arising from frequent opinion exchange within the cluster; 5) the system collapses into a global consensus with a moderate position after the long-time persistence of one integrated opinion cluster; 6) the remark that strengthening feedback can undoubtedly increase the likelihood of AP. For the first time, our study proposes a basic model framework to explore the unique dynamic features of AP.</p>
<p>The paper is organized as follows: in <xref ref-type="sec" rid="s2">Section 2</xref>, we formally define our opinion evolution model, along with the method to identify the regions of different states; in <xref ref-type="sec" rid="s3">Section 3</xref>, we simulate our model and give results, as well as descriptions and attempts to identify the unique dynamics features of AP. We conclude with a summary of the results and an outlook for future studies in <xref ref-type="sec" rid="s4">Section 4</xref>.</p>
</sec>
<sec id="s2">
<title>2 Model</title>
<p>The model considers a population of size <italic>N</italic> where each individual is typified by an opinion <italic>x</italic>
<sub>
<italic>i</italic>
</sub>(<italic>t</italic>) at time <italic>t</italic>, which is a real number in the interval <italic>x</italic>
<sub>
<italic>i</italic>
</sub>(<italic>t</italic>) &#x2208; [&#x2212;10, &#x2b; 10]. We adopt the opinion model proposed by [<xref ref-type="bibr" rid="B39">39</xref>], where the updating rules of an individual&#x2019;s opinion <italic>x</italic>
<sub>
<italic>i</italic>
</sub>(<italic>t</italic>) are formulated by the following equations:<disp-formula id="e1">
<mml:math id="m1">
<mml:msub>
<mml:mrow>
<mml:mover accent="true">
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
<mml:mo>&#x307;</mml:mo>
</mml:mover>
</mml:mrow>
<mml:mrow>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfenced>
<mml:mo>&#x3d;</mml:mo>
<mml:mfenced open="{" close="">
<mml:mrow>
<mml:mtable class="cases">
<mml:mtr>
<mml:mtd columnalign="left">
<mml:mi>A</mml:mi>
<mml:mo>&#x2061;</mml:mo>
<mml:mi>tanh</mml:mi>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>&#x3b1;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:msub>
<mml:msub>
<mml:mrow>
<mml:mi>D</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>j</mml:mi>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:mi>t</mml:mi>
</mml:mrow>
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<mml:mspace width="1em"/>
<mml:mtext>if</mml:mtext>
<mml:mspace width="0.3333em" class="nbsp"/>
<mml:mo stretchy="false">&#x7c;</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mi>D</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>j</mml:mi>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfenced>
<mml:mo stretchy="false">&#x7c;</mml:mo>
<mml:mo>&#x3c;</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mi>T</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>;</mml:mo>
<mml:mspace width="1em"/>
</mml:mtd>
</mml:mtr>
<mml:mtr>
<mml:mtd columnalign="left">
<mml:mi>A</mml:mi>
<mml:mo>&#x2061;</mml:mo>
<mml:mi>tanh</mml:mi>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>&#x3b1;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mi>&#x3c3;</mml:mi>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>D</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>j</mml:mi>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mfenced>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>T</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x2212;</mml:mo>
<mml:mo stretchy="false">&#x7c;</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mi>D</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>j</mml:mi>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfenced>
<mml:mo stretchy="false">&#x7c;</mml:mo>
</mml:mrow>
</mml:mfenced>
</mml:mrow>
</mml:mfenced>
<mml:mspace width="1em"/>
<mml:mtext>if</mml:mtext>
<mml:mspace width="0.3333em" class="nbsp"/>
<mml:mo stretchy="false">&#x7c;</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mi>D</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>j</mml:mi>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfenced>
<mml:mo stretchy="false">&#x7c;</mml:mo>
<mml:mo>&#x2265;</mml:mo>
<mml:msub>
<mml:mrow>
<mml:mi>T</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>.</mml:mo>
<mml:mspace width="1em"/>
</mml:mtd>
</mml:mtr>
</mml:mtable>
</mml:mrow>
</mml:mfenced>
</mml:math>
<label>(1)</label>
</disp-formula>
<italic>D</italic>
<sub>
<italic>ji</italic>
</sub>(<italic>t</italic>) &#x3d; <italic>x</italic>
<sub>
<italic>j</italic>
</sub>(<italic>t</italic>) &#x2212; <italic>x</italic>
<sub>
<italic>i</italic>
</sub>(<italic>t</italic>) denotes the opinion distance between <italic>i</italic> and <italic>j</italic> at time <italic>t</italic>. <italic>T</italic>
<sub>
<italic>i</italic>
</sub> is the tolerance threshold of an individual <italic>i</italic>. <italic>&#x3b1;</italic>
<sub>
<italic>i</italic>
</sub> can be interpreted as the response susceptibility of the individual. In more detail, <italic>&#x3b1;</italic>
<sub>
<italic>i</italic>
</sub> positively associates with the extent to which an individual <italic>i</italic> is passionate or sensitive, i.e., response susceptible to being socially influenced. It is obvious that the nonlinear shape of the influence function tanh(<italic>x</italic>) is controlled by <italic>&#x3b1;</italic>, while <italic>A</italic> quantifies the interaction strength, which is actually the upper bound of the opinion shift driven by each interaction, implying that the influence exerted by individuals on others is capped. <italic>&#x3c3;</italic>(<italic>D</italic>
<sub>
<italic>ji</italic>
</sub>(<italic>t</italic>)) extracts the sign of <italic>D</italic>
<sub>
<italic>ji</italic>
</sub>(<italic>t</italic>).</p>
<p>We first consider a population where the connections of each individual are dynamic and formulated by the activity-driven (AD) model [<xref ref-type="bibr" rid="B40">40</xref>&#x2013;<xref ref-type="bibr" rid="B43">43</xref>]. In more detail, <italic>k</italic>
<sub>
<italic>i</italic>
</sub>(<italic>t</italic>) denotes the number of interactions an individual <italic>i</italic> has at time <italic>t</italic>. It, thus, generates a temporal network formulated by the temporal adjacency matrix <italic>A</italic>
<sub>
<italic>ij</italic>
</sub>(<italic>t</italic>), where <italic>A</italic>
<sub>
<italic>ij</italic>
</sub>(<italic>t</italic>) &#x3d; 1 if an individual <italic>i</italic> owns one connection with an individual <italic>j</italic>; otherwise, <italic>A</italic>
<sub>
<italic>ij</italic>
</sub>(<italic>t</italic>) &#x3d; 0. Within the AD model framework, each individual <italic>i</italic> randomly connects <italic>k</italic>
<sub>
<italic>i</italic>
</sub> individuals from the population at each time step. <inline-formula id="inf1">
<mml:math id="m2">
<mml:msub>
<mml:mrow>
<mml:mi>k</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:msubsup>
<mml:mrow>
<mml:mo movablelimits="false" form="prefix">&#x2211;</mml:mo>
</mml:mrow>
<mml:mrow>
<mml:mi>j</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>N</mml:mi>
</mml:mrow>
</mml:msubsup>
<mml:msub>
<mml:mrow>
<mml:mi>A</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>i</mml:mi>
<mml:mi>j</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mi>t</mml:mi>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:math>
</inline-formula> is thus satisfied throughout the simulation. The evolution of opinions is actually coupled to an underlying temporal network. In reality, the empirical statistics show that the interaction activities of people are generally heterogeneous [<xref ref-type="bibr" rid="B29">29</xref>,<xref ref-type="bibr" rid="B41">41</xref>,<xref ref-type="bibr" rid="B42">42</xref>,<xref ref-type="bibr" rid="B44">44</xref>]. We, thus, further assume the interactions are extracted from a power-law distribution <italic>p</italic>(<italic>k</italic>) &#x223c; <italic>k</italic>
<sup>&#x2212;<italic>&#x3b3;</italic>
</sup>.</p>
<p>The proposed model incorporates the micronegative feedback mechanism by which individuals with more extreme opinions become more stubborn and less sensitive, making it more difficult to reposition. The micro feedback mechanism with regards to affective decision-making is based on the individual level and related to intrinsic preferences. On the basis of the basic model defined by Eq. <xref ref-type="disp-formula" rid="e1">1</xref>, we additionally assume the following feedback function regarding either interaction susceptibility <italic>&#x3b1;</italic>, using the individual opinion as the variable:<disp-formula id="e2">
<mml:math id="m3">
<mml:msub>
<mml:mrow>
<mml:mi>&#x3b1;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>i</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfenced>
<mml:mo>&#x3d;</mml:mo>
<mml:mi>&#x3b7;</mml:mi>
<mml:msubsup>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>i</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:mi>&#x3b2;</mml:mi>
</mml:mrow>
</mml:msubsup>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:mi>t</mml:mi>
</mml:mrow>
</mml:mfenced>
<mml:mo>,</mml:mo>
</mml:math>
<label>(2)</label>
</disp-formula>where <italic>&#x3b2;</italic> quantifies the strength of the negative feedback. The larger <italic>&#x3b2;</italic>, the stronger the feedback becomes, and as a consequence, even moderate individuals will not change their position easily. The feedback function captures the coupled relationship between individuals&#x2019; opinions and their preferences. This means that the present model includes intrinsic preferences for a specific opinion. Varying <italic>&#x3b2;</italic> may generate different evolution dynamics, facilitating an understanding of the effects of the micro feedback on the emergent dynamics of global polarization, global consensus, and &#x201c;harmony with diversity&#x201d; (HD) states.</p>
<p>Next, we extend the proposed model from the AD network to the static network where the interactions among individuals are fixed, such as the parts of the online social network Facebook. In such a case, <italic>k</italic>
<sub>
<italic>i</italic>
</sub> corresponds to the number of edges that the individual <italic>i</italic> stretches to its neighbors, and the individual is represented by a node in the networks. Therefore, the ones with which each individual interacts remain unchanged.</p>
<p>In numerical simulations, the size of the used time-varying network is <italic>N</italic> &#x3d; 1000, where <italic>&#x3b3;</italic> &#x3d; 2.1. The control parameters of the present model are <italic>A</italic>, <italic>&#x3b2;</italic>, and <italic>T</italic>
<sub>
<italic>i</italic>
</sub>, where we assume that individuals have uniform attributes <italic>&#x3b1;</italic>
<sub>
<italic>i</italic>
</sub> &#x3d; <italic>&#x3b1;</italic>, <italic>T</italic>
<sub>
<italic>i</italic>
</sub> &#x3d; <italic>T,</italic> and <italic>A</italic>
<sub>
<italic>i</italic>
</sub> &#x3d; <italic>A</italic>. For simplicity, we set <italic>&#x3b7;</italic> &#x3d; 1.0. The final results are obtained from <italic>N</italic>
<sub>
<italic>r</italic>
</sub> &#x3d; 100&#x2013;500 independent realizations, after at least 500 time steps. Before starting each realization, the initial opinion of each individual is independently and randomly sampled from the interval [&#x2212;1.0, 1.0]. Then, at each time step <italic>t</italic>, opinion evolves as follows: i) in a random order, each individual <italic>i</italic> randomly chooses <italic>k</italic>
<sub>
<italic>i</italic>
</sub> new neighbors out of all individuals, while the neighbors of <italic>i</italic> remain unchanged in the static social media network. ii) Then, <italic>i</italic> compares its opinion with each neighbor, attempting to update its opinion according to Eq. <xref ref-type="disp-formula" rid="e1">1</xref>, with adaptive response susceptibility <italic>&#x3b1;</italic>(<italic>x</italic>
<sub>
<italic>i</italic>
</sub> (<italic>t</italic> &#x2212; 1)) defined by Eq. <xref ref-type="disp-formula" rid="e2">2</xref>.</p>
<p>We exhibit the polarization dynamics through the polarization degree of a population, which is measured by the standard deviation (SD) in opinions <italic>SD</italic> (<italic>x</italic>
<sub>0</sub>, &#x2026; , <italic>x</italic>
<sub>
<italic>N</italic>
</sub>). We measure the opinion diversity by calculating the opinion entropy <italic>S</italic>) of the population Cui [<xref ref-type="bibr" rid="B39">39</xref>], <inline-formula id="inf2">
<mml:math id="m4">
<mml:mi>S</mml:mi>
<mml:mo>&#x3d;</mml:mo>
<mml:msubsup>
<mml:mrow>
<mml:mo movablelimits="false" form="prefix">&#x2211;</mml:mo>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi mathvariant="italic">min</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi mathvariant="italic">max</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
</mml:msubsup>
<mml:mi>x</mml:mi>
<mml:msub>
<mml:mrow>
<mml:mi>&#x3c1;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
</mml:math>
</inline-formula>, so as to capture the emergence of the HD state. <inline-formula id="inf3">
<mml:math id="m5">
<mml:msub>
<mml:mrow>
<mml:mi>&#x3c1;</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msub>
<mml:mrow>
<mml:mi>N</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mi>x</mml:mi>
</mml:mrow>
</mml:msub>
</mml:mrow>
<mml:mrow>
<mml:mi>N</mml:mi>
</mml:mrow>
</mml:mfrac>
</mml:math>
</inline-formula> is the density of the individual owning opinion <italic>x</italic>, and <italic>N</italic>
<sub>
<italic>x</italic>
</sub> denotes the population of the opinion <italic>x</italic>. Therefore, <italic>x</italic>
<italic>
<sub>min</sub>
</italic> &#x3d; &#x2212;10 and <italic>x</italic>
<italic>
<sub>max</sub>
</italic> &#x3d; 10 in our model. A larger <italic>SD</italic> indicates an increased degree of polarization. For example, the minimum of the polarization is zero, i.e., <italic>SD</italic>
<italic>
<sub>min</sub>
</italic> &#x3d; 0, corresponding to the GC state. Otherwise, the system will get extremely polarized if <italic>SD</italic> is large or equal to <italic>SD</italic>
<italic>
<sub>max</sub>
</italic> &#x3d; 10.</p>
<p>Inspired by the phase-identification method developed in [<xref ref-type="bibr" rid="B39">39</xref>], we still numerically estimate the boundaries between different states by means of the susceptibility of not only <italic>S</italic> but also <italic>SD</italic>.<disp-formula id="e3">
<mml:math id="m6">
<mml:mi>&#x3c7;</mml:mi>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:mi>S</mml:mi>
</mml:mrow>
</mml:mfenced>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msqrt>
<mml:mrow>
<mml:mrow>
<mml:mo stretchy="false">&#x27e8;</mml:mo>
<mml:mrow>
<mml:msup>
<mml:mrow>
<mml:mi>S</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
<mml:mo stretchy="false">&#x27e9;</mml:mo>
</mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mrow>
<mml:mo stretchy="false">&#x27e8;</mml:mo>
<mml:mrow>
<mml:mi>S</mml:mi>
</mml:mrow>
<mml:mo stretchy="false">&#x27e9;</mml:mo>
</mml:mrow>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:msqrt>
</mml:mrow>
<mml:mrow>
<mml:mrow>
<mml:mo stretchy="false">&#x27e8;</mml:mo>
<mml:mrow>
<mml:mi>S</mml:mi>
</mml:mrow>
<mml:mo stretchy="false">&#x27e9;</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:mfrac>
<mml:mo>,</mml:mo>
</mml:math>
<label>(3)</label>
</disp-formula>
<disp-formula id="e4">
<mml:math id="m7">
<mml:mi>&#x3c7;</mml:mi>
<mml:mfenced open="(" close=")">
<mml:mrow>
<mml:mi>S</mml:mi>
<mml:mi>D</mml:mi>
</mml:mrow>
</mml:mfenced>
<mml:mo>&#x3d;</mml:mo>
<mml:mfrac>
<mml:mrow>
<mml:msqrt>
<mml:mrow>
<mml:mrow>
<mml:mo stretchy="false">&#x27e8;</mml:mo>
<mml:mrow>
<mml:msup>
<mml:mrow>
<mml:mi>S</mml:mi>
<mml:mi>D</mml:mi>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
<mml:mo stretchy="false">&#x27e9;</mml:mo>
</mml:mrow>
<mml:mo>&#x2212;</mml:mo>
<mml:msup>
<mml:mrow>
<mml:mrow>
<mml:mo stretchy="false">&#x27e8;</mml:mo>
<mml:mrow>
<mml:mi>S</mml:mi>
<mml:mi>D</mml:mi>
</mml:mrow>
<mml:mo stretchy="false">&#x27e9;</mml:mo>
</mml:mrow>
</mml:mrow>
<mml:mrow>
<mml:mn>2</mml:mn>
</mml:mrow>
</mml:msup>
</mml:mrow>
</mml:msqrt>
</mml:mrow>
<mml:mrow>
<mml:mrow>
<mml:mo stretchy="false">&#x27e8;</mml:mo>
<mml:mrow>
<mml:mi>S</mml:mi>
<mml:mi>D</mml:mi>
</mml:mrow>
<mml:mo stretchy="false">&#x27e9;</mml:mo>
</mml:mrow>
</mml:mrow>
</mml:mfrac>
<mml:mo>,</mml:mo>
</mml:math>
<label>(4)</label>
</disp-formula>where &#x27e8;<italic>S</italic>&#x27e9; (&#x27e8;&#x2009;<italic>SD</italic>&#x2009;&#x27e9;) is the ensemble average of <italic>S</italic> (<italic>SD</italic>), which can be obtained by averaging <italic>S</italic> (<italic>SD</italic>) from <italic>N</italic>
<sub>
<italic>r</italic>
</sub> independent realizations. &#x27e8;<italic>S</italic>
<sup>2</sup>&#x27e9; (&#x27e8;&#x2009;<italic>SD</italic>
<sup>2</sup>&#x27e9;) is the secondary moment of the ensemble distribution. One can further identify the boundaries between GC, HD, and AP states according to the principle that <italic>&#x3c7;</italic>(<italic>S</italic>) and <italic>&#x3c7;</italic>(<italic>SD</italic>) exhibit a peak value at the boundary.</p>
</sec>
<sec sec-type="results" id="s3">
<title>3 Results</title>
<p>
<xref ref-type="fig" rid="F1">Figures 1</xref>, <xref ref-type="fig" rid="F2">2</xref> present the temporal evolution of the individuals&#x2019; opinions, polarization degree <italic>SD</italic>, and opinion entropy <italic>S</italic> for six different parameter conditions, respectively. Corresponding final opinion distributions are illustrated in <xref ref-type="fig" rid="F3">Figure 3</xref>. We can observe that as the interaction strength <italic>A</italic> increases, the system first shifts from HD to GC, then from GC to the AP state. More in detail, the presence of opinion-based feedback can facilitate stable integrated opinion cluster centering on a neutral point (see <xref ref-type="fig" rid="F1">Figure 1A</xref>), along with stable considerable <italic>S</italic> and low-level <italic>SD</italic> (see <xref ref-type="fig" rid="F2">Figure 2A</xref>). Since individuals are allowed to remain greatly sensitive to the diverse views of others in spite of their opinion distance being slight (see <xref ref-type="sec" rid="s10">Supplementary Figure S1A</xref>), this occurs in frequent opinion exchanges because of both being rather sensitive and have weak mutual attraction [<xref ref-type="bibr" rid="B39">39</xref>], further leading to persisting violently oscillating average susceptibility (see <xref ref-type="sec" rid="s10">Supplementary Figure S1A</xref>). In such cases, the system does not easily get trapped in a monotonous state such as GC or AP. Moreover, this cluster exhibits a much more stable trajectory in comparison with <xref ref-type="fig" rid="F1">Figure 1</xref> in [<xref ref-type="bibr" rid="B39">39</xref>], in which the coupled feedback is not considered, showing one advantage of this feedback.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption>
<p>Temporal evolution of the individuals&#x2019; opinions for six different representative values of A are presented in <bold>(A&#x2013;F)</bold>, respectively. They are also indicated by the dark green dots in <xref ref-type="fig" rid="F4">Figures 4A1, A2</xref>, for a more explicit presentation. The values of the parameters are listed in the titles of the subplots.</p>
</caption>
<graphic xlink:href="fphy-11-1213044-g001.tif"/>
</fig>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption>
<p>Temporal evolution of <italic>SD</italic> and <italic>S</italic> for six different representative values of A are presented in <bold>(A&#x2013;F)</bold>, respectively. The six representative cases are also indicated by the dark green dots in <xref ref-type="fig" rid="F4">Figures 4A1, A2</xref>, for a more explicit presentation. The values of the parameters are the same, as considered in <xref ref-type="fig" rid="F1">Figure 1</xref>.</p>
</caption>
<graphic xlink:href="fphy-11-1213044-g002.tif"/>
</fig>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption>
<p>Final opinion distributions of the population for six different representative values of A are presented in <bold>(A&#x2013;F)</bold>, respectively. The values of parameters are listed in the titles of the subfigures, corresponding to the six cases illustrated in <xref ref-type="fig" rid="F1">Figures 1, 2</xref>.</p>
</caption>
<graphic xlink:href="fphy-11-1213044-g003.tif"/>
</fig>
<p>However, the intermediate <italic>A</italic> instead gives rise to the GC state, in which the integrated cluster collapses and converges into a single moderate position from which it would never move (see <xref ref-type="fig" rid="F1">Figures 1B, C</xref>), exhibiting sudden drops of <italic>S</italic> and <italic>SD</italic> (see <xref ref-type="fig" rid="F2">Figures 2B, C</xref>). Intermediate interaction strength brings about a wider opinion spectrum and, thus, more insensitive and insistent individuals in the presence of the feedback, who can hold a more stable position. In addition, at the stage of the opinion cluster, the opinion distances between individuals are mostly within <italic>T</italic> before the collapse. The aforementioned two factors contribute to a global consensus as sharply as possible. It is, thus, also evidence for the existence of the dynamic equilibrium. Attributing to rather small <inline-formula id="inf4">
<mml:math id="m8">
<mml:mrow>
<mml:mover accent="true">
<mml:mrow>
<mml:mi>&#x3b1;</mml:mi>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mi>t</mml:mi>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mrow>
<mml:mo>&#x304;</mml:mo>
</mml:mover>
</mml:mrow>
</mml:math>
</inline-formula> (see <xref ref-type="sec" rid="s10">Supplementary Figures S1B, C</xref>), individuals become rather slow as the population achieves a high degree of consensus. Remarkably, we can see in <xref ref-type="fig" rid="F3">Figures 3B, C</xref> that the convergence point is not always neutral where all individuals maintain perfect neutrality. The system is definitely initial condition-dependent, which may result from the initial unequal distribution of individuals with opinions on different signs. In such cases, the convergence direction is uncertain. It is hard to achieve a global consensus with a neutral point when coupled feedback is present.</p>
<p>As <italic>A</italic> gets larger, individuals will not keep an open attitude toward distant ones due to strong repulsive forces caused by strong interaction. The population may get polarized with large <italic>SD</italic>, which is, however, less than <italic>SD</italic>
<italic>
<sub>max</sub>
</italic> (i.e., high-level AP rather than extreme AP). In such cases, the population evolves into two opposite camps of different sizes (see asymmetric opinion distributions illustrated in <xref ref-type="fig" rid="F3">Figures 3D, E</xref>), which, thus, belongs to an asymmetric class [<xref ref-type="bibr" rid="B45">45</xref>,<xref ref-type="bibr" rid="B46">46</xref>]. The opinions of the majority population may first self-organize into one integrated cluster to confront the repulsive force, which can leave the moderates within the tolerance range. However, the repulsion from the opposing stubborn extremists caused by the feedback is superior to their mutual attraction, which will reinforce and shift the cluster until the opinion boundaries absorb it (see <xref ref-type="fig" rid="F1">Figures 1D, E</xref>). As another result, we observe a three-step trajectory of <italic>S</italic> (see <xref ref-type="fig" rid="F2">Figures 2D, E</xref> and a slowly decreasing <inline-formula id="inf5">
<mml:math id="m9">
<mml:mrow>
<mml:mover accent="true">
<mml:mrow>
<mml:mi>&#x3b1;</mml:mi>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mi>t</mml:mi>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mrow>
<mml:mo>&#x304;</mml:mo>
</mml:mover>
</mml:mrow>
</mml:math>
</inline-formula> after an intensive drop (see <xref ref-type="sec" rid="s10">Supplementary Figures S1D, E</xref>), indicating the occurrence of a dynamic equilibrium. The system actually enters a transient stage. The occurrence of the dynamic equilibrium has never been uncovered in previous studies, especially those considering interactions based on bounded confidence. With increasing <italic>A</italic>, high-level polarization would be replaced by symmetric extreme polarization with <italic>SD &#x2248;</italic> <italic>SD<sub>max</sub>
</italic> (see <xref ref-type="fig" rid="F1">Figures 1F</xref>, <xref ref-type="fig" rid="F2">2F</xref>, <xref ref-type="fig" rid="F3">3F</xref>). The cluster can be symmetrically torn apart within a short time (see <xref ref-type="fig" rid="F1">Figure 1F</xref>), due to the strong repulsive forces arising from the strong interaction [<xref ref-type="bibr" rid="B39">39</xref>]. This makes the prior self-organization into one majority cluster impossible, and individuals become quickly insensitive (see <xref ref-type="sec" rid="s10">Supplementary Figure S1F</xref>) for <inline-formula id="inf6">
<mml:math id="m10">
<mml:mrow>
<mml:mover accent="true">
<mml:mrow>
<mml:mi>&#x3b1;</mml:mi>
<mml:mrow>
<mml:mo stretchy="false">(</mml:mo>
<mml:mrow>
<mml:mi>t</mml:mi>
</mml:mrow>
<mml:mo stretchy="false">)</mml:mo>
</mml:mrow>
</mml:mrow>
<mml:mo>&#x304;</mml:mo>
</mml:mover>
</mml:mrow>
<mml:mo>&#x2248;</mml:mo>
<mml:mn>0</mml:mn>
</mml:math>
</inline-formula>).</p>
<p>
<xref ref-type="fig" rid="F4">Figure 4</xref> presents a more clear dependence of <italic>SD</italic>, <italic>S,</italic> and <italic>&#x3c7;</italic>(<italic>S</italic>) on interaction strength <italic>A</italic> and tolerance threshold <italic>T</italic>. It is obvious in <xref ref-type="fig" rid="F4">Figures 4A1, A2</xref> that increasing <italic>A</italic> has an obvious nonlinear effect on both the polarization degree <italic>SD</italic> and opinion diversity, i.e., opinion entropy <italic>S</italic>. The range of weak interactions <italic>A</italic> &#x3c; <italic>A</italic>
<sub>
<italic>c</italic>1</sub> is for the emergence of HD states, showing small <italic>SD</italic> and highland of <italic>S</italic>. We have also checked that the spectrum width of the cluster is positively related to the value of <italic>S</italic>, while the system governed by the intermediate range <italic>A</italic>
<sub>
<italic>c</italic>1</sub> &#x3c; <italic>A</italic> &#x3c; <italic>A</italic>
<sub>
<italic>c</italic>2</sub> provides sufficient evidence for a GC state with <italic>SD</italic> &#x3d; 0 and <italic>S</italic> &#x3d; 0. This is definitely in contrast to the emergent properties generated by the attraction&#x2013;repulsion model without consideration of feedback [<xref ref-type="bibr" rid="B39">39</xref>], in which a dynamic balance is responsible for the emergence of HD states. Similar behaviors can be observed in <xref ref-type="fig" rid="F4">Figures 4B1, B2</xref>, while <xref ref-type="fig" rid="F4">Figures 4C1, C2</xref> reveal that the system undergoes a shift from AP to the HD state with increasing tolerance threshold <italic>T</italic>. This is largely in accordance with the empirical evidence [<xref ref-type="bibr" rid="B47">47</xref>,<xref ref-type="bibr" rid="B48">48</xref>] and the social moral rules requiring a high-level of tolerance, essentially attempting to achieve an HD state. In addition, it should be noticed that the peaks of <italic>&#x3c7;</italic>(<italic>S</italic>) correspond rightly to the critical points between these phases, which further validate the phase-identification method developed in [<xref ref-type="bibr" rid="B39">39</xref>].</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption>
<p>In time-varying networks, dependence of <italic>SD</italic> (red circles) and <italic>&#x03C7;</italic>(<italic>S</italic>) (black triangles) on A are presented in <bold>(A1, B1)</bold>, while dependence of S (blue squares) and <italic>&#x03C7;</italic>(<italic>S</italic>) (black triangles) on A are presented in <bold>(A2, B2)</bold>. In <bold>(C1, C2)</bold>, we plot the dependence of dependence of <italic>SD</italic> (red circles) and <italic>&#x03C7;</italic>(<italic>S</italic>) (black triangles) on <italic>T</italic>, and the dependence of dependence of <italic>S</italic> (blue squares) and <italic>&#x03C7;</italic>(<italic>S</italic>) (black triangles) on <italic>T</italic>, respectively. In <bold>(A1, A2)</bold>, the six dark green dots correspond to the subplots of six parameter combinations in <xref ref-type="fig" rid="F1">Figures 1&#x2013;3</xref>. In <bold>(A)</bold> and <bold>(B)</bold>, pink vertical lines label the positions of <italic>A<sub>c1</sub>
</italic> at which the GC state begins to appear, while light blue vertical lines indicate the positions of <italic>A<sub>c2</sub>
</italic> at which the GC state starts to vanish and shift to the AP state. However, we can observe in (<italic>C1</italic>) and (<italic>C2</italic>) that the threshold <italic>T<sub>c</sub>
</italic> that denotes a shift from AP to HD. The values of parameters are correspondingly listed in the titles of subfigures.</p>
</caption>
<graphic xlink:href="fphy-11-1213044-g004.tif"/>
</fig>
<p>We next extend the simulations to (<italic>A</italic>, <italic>T</italic>) space, as shown in <xref ref-type="fig" rid="F5">Figure 5</xref>, where the color encodes the values of <italic>SD</italic> for four different representative values of feedback strength <italic>&#x3b2;</italic>. The system finally evolves into either HD or AP state when <italic>&#x3b2;</italic> is small such that there is only one transition from HD to AP. When <italic>&#x3b2;</italic> increases to some extent (<italic>&#x3b2;</italic> &#x3d; 2.0), the intermediate range of <italic>A</italic> can additionally lead to the emergence of the GC state for sufficient tolerance and the triple points (see the blue or black pentagrams illustrated in <xref ref-type="fig" rid="F5">Figures 5B, D</xref>). Therefore, we can observe three different transitions by increasing <italic>A</italic>: from HD to GC, which is largely dependent on <italic>A</italic>, from GC to AP and from HD to AP when <italic>&#x3b2;</italic> is larger than a certain value. For all strong feedback, GC is promoted to erode the regions of HD, and in turn, AP occupies the regions of GC, leading to the shrinkage of HD regions. However, both increasing <italic>T</italic> and decreasing <italic>A</italic> can prevent the population from being polarized as much as possible for a given <italic>&#x3b2;</italic>. However, we find that strong feedback is responsible for the decreasing polarization degree, such that extreme AP is widely replaced by high-level AP (see <xref ref-type="fig" rid="F5">Figure 5D</xref>). The strong stubbornness of individuals (small <italic>&#x03B1;</italic>
<sub>i</sub>), as well as the strengthening interactions bringing about intense struggles between individuals of different signs, contribute to the self-organization into one integrated cluster which gradually approaches the boundary (see <xref ref-type="fig" rid="F5">Figures 1D, E</xref>), i.e., the dynamic equilibrium.</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption>
<p>Phase diagrams in terms of <italic>SD</italic> are presented in (<italic>A, T</italic>) space for four different values of <italic>&#x03B2;</italic>: <bold>(A)</bold> <italic>&#x03B2;</italic> &#x003D; 0.8, <bold>(B)</bold> <italic>&#x03B2;</italic> &#x003D; 2.0, <bold>(C)</bold> <italic>&#x03B2;</italic> &#x003D; 4.0 and <bold>(D)</bold> <italic>&#x03B2;</italic> &#x003D; 6.0. The lines consisting of pink triangles separate the regions of HD and GC phases, while the lines consisting of yellow circles depict the boundaries indicated by the second threshold <italic>A<sub>c2</sub>
</italic>, separating the regions of the HD and P phases, as given by our method. The lines consisting of brown diamonds separate the regions of the GC and P phases. The regions belonging to different states are labeled in the subplots. In particular, the light blue pentagrams illustrated in <bold>(B&#x2013;D)</bold> indicate the triple points.</p>
</caption>
<graphic xlink:href="fphy-11-1213044-g005.tif"/>
</fig>
<p>
<xref ref-type="fig" rid="F6">Figure 6</xref> depicts the phase diagrams in (<italic>A</italic>, <italic>&#x3b2;</italic>) space. By increasing <italic>A</italic>, there still occur three transitions when individuals are sufficiently tolerant (see <xref ref-type="fig" rid="F6">Figures 6B, D</xref>): the transition from HD to AP occurs with weak feedback, whereas strong feedback is favorable for the other two transitions: from GC to AP and from HD to GC. It suggests that the interaction strength <italic>A</italic> plays a decisive role, while larger light red regions of AP (see <xref ref-type="fig" rid="F6">Figure 6</xref>) further confirm that strong feedback may prevent the system from getting extremely polarized and facilitate GC by suppressing HD, which, however, becomes dominant for small <italic>&#x3b2;</italic> and <italic>A</italic>, but large <italic>T</italic>.</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption>
<p>Phase diagrams in terms of <italic>SD</italic> are presented in <italic>(A, &#x03B2;)</italic> space for four different values of <italic>T</italic>: <bold>(A)</bold> <italic>T</italic> &#x003D; 1.0, <bold>(B)</bold> <italic>T</italic> &#x003D; 4.0, <bold>(C)</bold> <italic>T</italic> &#x003D; 7.0 and <bold>(D)</bold> <italic>T</italic> &#x003D; 10.0. The lines consisting of pink triangles separate the regions of GC and HD phases, while the lines consisting of yellow circles depict the boundaries indicated by the second threshold <italic>A<sub>c2</sub>
</italic>, separating the regions of HD and P phases, as given by our method. The lines consisting of brown diamonds separate the regions of the GC and P phases. The regions belonging to different states are labeled in the subplots. In particular, the light blue pentagram illustrated in <bold>(B)</bold> indicates one triple point. The four dots correspond to the subplots of the six parameter combinations in <xref ref-type="fig" rid="F1">Figure 1</xref>.</p>
</caption>
<graphic xlink:href="fphy-11-1213044-g006.tif"/>
</fig>
<p>
<xref ref-type="fig" rid="F7">Figure 7</xref> offers a comprehensive view of the effects of individuals&#x2019; tolerance on opinion dynamics for different levels of feedback. There is not only one transition from HD to GC with increasing <italic>&#x3b2;</italic> but also two novel transitions with increasing <italic>T</italic>: from AP to HD and from AP to GC. We find that, if <italic>A</italic> is not small, AP is likely to emerge for small <italic>T</italic>, whose regions expand with <italic>A</italic>, along with decreasing likelihood of HD and GC, while increasing both <italic>T</italic> and <italic>&#x3b2;</italic> is responsible for the GC state. In addition, sufficiently tolerant individuals and weak interactions are essential to easily achieving the HD state. Still, the system can generate triple points in such a parameter space.</p>
<fig id="F7" position="float">
<label>FIGURE 7</label>
<caption>
<p>Phase diagrams in terms of <italic>SD</italic> are presented in <italic>(T, &#x03B2;)</italic> space for four different values of <italic>A</italic>: <bold>(A)</bold> <italic>A</italic> &#x003D; 0.5, <bold>(B)</bold> <italic>A</italic> &#x003D; 1.0, <bold>(C)</bold> <italic>A</italic> &#x003D; 2.0 and <bold>(D)</bold> <italic>A</italic> &#x003D; 3.0. The lines consisting of pink triangles separate the regions of the GC and HD phases, while the lines consisting of yellow circles depict the boundaries indicated by the second threshold <italic>A<sub>c2</sub>
</italic>, separating the regions of HD and P phases, as given by our method. The lines consisting of brown diamonds separate the regions of GC and P phases. The regions belonging to different states are labeled in the subplots, while the light blue pentagrams indicate the existence of triple points.</p>
</caption>
<graphic xlink:href="fphy-11-1213044-g007.tif"/>
</fig>
<p>Overall, <xref ref-type="fig" rid="F5">Figures 5</xref>&#x2013;<xref ref-type="fig" rid="F7">7</xref> further confirm that AP may increase with strengthening feedback, particularly with low tolerance and strong interaction. It supports the researchers&#x2019; worry that political polarization among the US public may increase due to the AP and the coupled relationship between people&#x2019;s views and their response sensitivity [<xref ref-type="bibr" rid="B15">15</xref>,<xref ref-type="bibr" rid="B33">33</xref>&#x2013;<xref ref-type="bibr" rid="B35">35</xref>]. In addition, the phase-identification method allows us to build phase diagrams and locate where the triple points are, by identifying the boundaries between different phases.</p>
<p>Online social networks are increasingly used to access the formation dynamics of opinions with respect to COVID-19 vaccines, gun-control, and abortion [<xref ref-type="bibr" rid="B29">29</xref>,<xref ref-type="bibr" rid="B30">30</xref>,<xref ref-type="bibr" rid="B49">49</xref>,<xref ref-type="bibr" rid="B50">50</xref>]. These platforms can reduce barriers and costs to information and, further, allow individuals to freely voice their viewpoints, consequently improving the rate of opinion exchanges. We, thus, subsequently embed our model into the social networks where individuals interact through fixed connections so as to explore whether the topology of fixed connections can result in changes in opinion evolution dynamics. Still, similar phase diagrams are presented in <xref ref-type="fig" rid="F8">Figure 8</xref> in three different parameter spaces, (<italic>A</italic>, <italic>T</italic>), (<italic>A</italic>, <italic>&#x3b2;</italic>) and (<italic>T</italic>, <italic>&#x3b2;</italic>), suggesting that evolution outcomes are mainly dominated by the model rules rather than the structure of used networks. At the same time, a comparison between <xref ref-type="fig" rid="F5">Figures 5</xref>&#x2013;<xref ref-type="fig" rid="F8">8</xref> reveals that the introduction of fixed interactions can remarkably give rise to much larger high-level AP, which is actually attributed to the existence of cluster-level self-reinforced mechanisms (see <xref ref-type="sec" rid="s10">Supplementary Figure S2</xref>) [<xref ref-type="bibr" rid="B39">39</xref>]. As another result, both weak feedback and high-level tolerance promote GC regions to erode the regions of HD and to split them into two parts (see <xref ref-type="fig" rid="F8">Figures 8A1, B2&#x2013;B4</xref>). In such cases, individuals are generally within the stable clusters and moderately sensitive. However, the existence of these clusters can prevent them from contacting and struggling with those of dissimilar opinions, and, in turn, exert a persistent neutralizing influence on the prejudiced opinions on the boundaries because they are highly tolerant, regardless of the fact that they are relatively insensitive. Consequently, opinion exchanges are less frequent to maintain more stable opinions, and the GC state can be more easily achieved.</p>
<fig id="F8" position="float">
<label>FIGURE 8</label>
<caption>
<p>Phase diagram for the population embedded on the part of Facebook network, where interactions among individuals are fixed. <bold>(A1&#x2013;A3)</bold> Phase diagrams in (<italic>A</italic>, <italic>T</italic>) space for four different values of <italic>&#x3b2;</italic>. <bold>(B1&#x2013;B4)</bold> Phase diagram in (<italic>A</italic>, <italic>&#x3b2;</italic>) space for four different values of <italic>T</italic>. <bold>(C1&#x2013;C4)</bold> Phase diagram in (<italic>T</italic>, <italic>&#x3b2;</italic>) space for four different values of <italic>A</italic>. We run simulations with <italic>SD</italic> in all subplots. The lines consisting of different markers denote the boundaries between different phases, which are the same as those presented in <xref ref-type="fig" rid="F5">Figure 5</xref>. The regions of the three phases are correspondingly labeled in the subplots. The light blue pentagrams indicate the triple points, which are more frequent. The degree distribution of the used network is <italic>p</italic>
<sub>
<italic>k</italic>
</sub> &#x223c; <italic>k</italic>
<sup>&#x2212;<italic>&#x3b3;</italic>
</sup> with <italic>&#x3b3;</italic> &#x3d;&#x2212;3.22. The other structural parameters are: <italic>N</italic> &#x3d;43,952, mean degree &#x27e8;<italic>k</italic>&#x27e9;&#x3d;8.30, &#x27e8;<italic>k</italic>
<sup>2</sup>&#x27e9;&#x3d;205.36, maximum degree <italic>k</italic>
<sub>max</sub> &#x3d;223, minimum degree <italic>k</italic>
<sub>min</sub> &#x3d;1, modularity is 0.59, clustering coefficient <italic>c</italic> &#x3d;0.12, and degree correlation coefficient <italic>r</italic> &#x2273;0.</p>
</caption>
<graphic xlink:href="fphy-11-1213044-g008.tif"/>
</fig>
</sec>
<sec id="s4">
<title>4 Discussions and conclusion</title>
<p>For the first time, this study introduced feedback to capture the coupled relationship between individuals&#x2019; opinions and their susceptibilities to the views of others, which has been verified to be a useful approach to the micro foundations of AP dynamics. This assumption allows us to explore the unique dynamic features of AP for the first time. The simulations on both time-varying and static social networks show that strong coupled feedback between individuals&#x2019; opinions and susceptibility, and strong interaction among narrow minded individuals facilitate the emergence of the AP state. Extreme views easily arise from strong interactions between intolerant individuals. Since strong stubbornness is responsible for the existence of considerable extremists who can exert persistent influence on the moderate interactions in the population. In contrast, weak interaction, high tolerance, and weak coupled feedback are favorable for HD states, which actually guide us on how to avoid the dilemmas caused by AP. Otherwise, strong stubbornness caused by extreme positions makes individuals stand out together to face the opposite of them. In addition, the simulations further confirm that the peak of entropy susceptibility is indeed a sign of transition between GC, HD, and AP states [<xref ref-type="bibr" rid="B39">39</xref>].</p>
<p>However, intermediate ranges of parameters yield the GC state, which emerges along with that one integrated cluster, always collapses, and converges toward a moderate position after a long-time persistence, leading to sudden drops in both <italic>S</italic> and <italic>SD</italic>. It is the first remark. Moreover, the aforementioned results highlight the second remark that the negative coupled feedback actually offers a counterforce to establish an inversion of the regions between GC and HD, in comparison with the results presented in <xref ref-type="fig" rid="F4">Figures 4A1&#x2013;A4</xref>, which do not consider this feedback [<xref ref-type="bibr" rid="B39">39</xref>]. As the third remark suggests, stronger feedback measuring more emotional response can yield a high likelihood of polarization, which is in accordance with empirical investigations of affective polarization in the US [<xref ref-type="bibr" rid="B13">13</xref>,<xref ref-type="bibr" rid="B15">15</xref>,<xref ref-type="bibr" rid="B33">33</xref>,<xref ref-type="bibr" rid="B34">34</xref>]. Still, fixed connections can bring about cluster-level self-reinforced mechanisms which can enlarge the regions of high-level AP.</p>
<p>Moreover, as the fourth remark suggests coupled feedback with a large intermediate <italic>A</italic> may promote fast self-organization into one opinion cluster toward GC or even high-level AP. This cluster that does not remain robust against time is also responsible for the step-like dynamic behaviors of opinion entropy. In such cases, the system enters a transient stage, suggesting the existence of a dynamic equilibrium. In summary, the aforementioned four remarks cannot be identified by previous studies involving polarization issues; they are novel, unique dynamic features of AP within our model framework.</p>
<p>Our model is based on the simple assumption that interactions among similar actors will reduce their differences and that the opposite is true for interactions among distant actors. It is significant that future studies should take into account some empirical characteristics of individuals which might generate different scenarios, such as heterogeneous duration time of interactions, heterogeneous feedback strength, or different social positions. Moreover, the existence of prior self-organization into one integrated cluster before reaching the AP state may highlight a golden time window, in which regulation measures may most effectively prevent the public from reaching dangerous degrees of AP, which is also worth leaving this investigation to future research. Furthermore, empirical evidence to verify the conclusion of the present study is required. Moreover, this study opens up one interesting issue to identify the difference between AP and IP with respect to their emergent dynamics.</p>
</sec>
</body>
<back>
<sec sec-type="data-availability" id="s5">
<title>Data availability statement</title>
<p>The original contributions presented in the study are included in the article/<xref ref-type="sec" rid="s10">Supplementary Material</xref>; further inquiries can be directed to the corresponding author.</p>
</sec>
<sec id="s6">
<title>Author contributions</title>
<p>P-BC designed the model, proceeded with simulations and analysis, and wrote and edited the original manuscript.</p>
</sec>
<sec id="s7">
<title>Funding</title>
<p>This work was supported by the Key Program of the National Natural Science Foundation of China (Grant No. 71731002) and by the Guangdong Basic and Applied Basic Research Foundation (Grant No. 2021A1515011975).</p>
</sec>
<sec sec-type="COI-statement" id="s8">
<title>Conflict of interest</title>
<p>The author declares that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.</p>
</sec>
<sec sec-type="disclaimer" id="s9">
<title>Publisher&#x2019;s note</title>
<p>All claims expressed in this article are solely those of the authors and do not necessarily represent those of their affiliated organizations, or those of the publisher, the editors, and the reviewers. Any product that may be evaluated in this article, or claim that may be made by its manufacturer, is not guaranteed or endorsed by the publisher.</p>
</sec>
<sec id="s10">
<title>Supplementary material</title>
<p>The Supplementary Material for this article can be found online at: <ext-link ext-link-type="uri" xlink:href="https://www.frontiersin.org/articles/10.3389/fphy.2023.1213044/full#supplementary-material">https://www.frontiersin.org/articles/10.3389/fphy.2023.1213044/full&#x23;supplementary-material</ext-link>
</p>
<supplementary-material xlink:href="DataSheet1.PDF" id="SM1" mimetype="application/PDF" xmlns:xlink="http://www.w3.org/1999/xlink"/>
</sec>
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