Cluster Anticonsensus of Multiagent Systems Based on the <svg xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg" style="vertical-align:-2.73601pt;width:17.3375px;" id="M1" height="18.8375" version="1.1" viewBox="0 0 17.3375 18.8375" width="17.3375">
	
		
			<g transform="matrix(.022,-0,0,-.022,.062,15.012)"><path id="x1D444" d="M745 361q0 -134 -83.5 -233t-214.5 -130l16 -11q97 -67 250 -132l-8 -23q-76 3 -131 16q-81 19 -242 125l-20 13q-129 8 -209 91t-80 208q0 160 116 271t289 111q136 0 226.5 -83t90.5 -223zM645 356q0 127 -57.5 201.5t-169.5 74.5q-126 0 -210.5 -104.5t-84.5 -248.5
q0 -97 46 -166.5t129 -87.5l84 15l29 -19q104 21 169 121.5t65 213.5z"></path></g>

		
	
</svg>-Theory

<table>Herschel graph: bipartite style.</table>

Discrete Dynamics in Nature and Society

fig2

Figure 2

Figure 2: Cluster Anticonsensus of Multiagent Systems Based on the <svg xmlns:xlink="http://www.w3.org/1999/xlink" xmlns="http://www.w3.org/2000/svg" style="vertical-align:-2.73601pt;width:17.3375px;" id="M1" height="18.8375" version="1.1" viewBox="0 0 17.3375 18.8375" width="17.3375">
	
		
			<g transform="matrix(.022,-0,0,-.022,.062,15.012)"><path id="x1D444" d="M745 361q0 -134 -83.5 -233t-214.5 -130l16 -11q97 -67 250 -132l-8 -23q-76 3 -131 16q-81 19 -242 125l-20 13q-129 8 -209 91t-80 208q0 160 116 271t289 111q136 0 226.5 -83t90.5 -223zM645 356q0 127 -57.5 201.5t-169.5 74.5q-126 0 -210.5 -104.5t-84.5 -248.5
q0 -97 46 -166.5t129 -87.5l84 15l29 -19q104 21 169 121.5t65 213.5z"></path></g>

		
	
</svg>-Theory 

Discrete Dynamics in Nature and Society

Cluster Anticonsensus of Multiagent Systems Based on the -Theory

Figure 2