Optimal community structure for social contagions

被引:12
|
作者
Su, Zhen [1 ,2 ]
Wang, Wei [3 ]
Li, Lixiang [4 ]
Stanley, H. Eugene [5 ,6 ]
Braunstein, Lidia A. [5 ,6 ,7 ]
机构
[1] Chongqing Univ Posts & Telecommun, Coll Comp Sci & Technol, Chongqing 400065, Peoples R China
[2] Chongqing MII Key Lab Comp Networks & Commun, Chongqing 400065, Peoples R China
[3] Sichuan Univ, Cybersecur Res Inst, Chengdu 610065, Sichuan, Peoples R China
[4] Beijing Univ Posts & Telecommun, Informat Secur Ctr, State Key Lab Networking & Switching Technol, Beijing 100876, Peoples R China
[5] Boston Univ, Ctr Polymer Studies, Boston, MA 02215 USA
[6] Boston Univ, Dept Phys, Boston, MA 02215 USA
[7] Univ Nacl Mar del Plata, CONICET, Fac Ciencias Exactas & Nat, Inst Invest Fis Mar del Plata IFIMAR,Dept Fis, Funes 3350, RA-7600 Mar Del Plata, Buenos Aires, Argentina
来源
NEW JOURNAL OF PHYSICS | 2018年 / 20卷
基金
美国国家科学基金会;
关键词
community structure; social contagions; nonlinear dynamics; COMPLEX NETWORKS; MULTILAYER NETWORKS; DYNAMICS; BEHAVIOR; CASCADES; PHYSICS; MODEL;
D O I
10.1088/1367-2630/aac0c9
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Community structure is an important factor in the behavior of real-world networks because it strongly affects the stability and thus the phase transition order of the spreading dynamics. We here propose a reversible social contagion model of community networks that includes the factor of social reinforcement. In our model an individual adopts a social contagion when the number of received units of information exceeds its adoption threshold. We use mean-field approximation to describe our proposed model, and the results agree with numerical simulations. The numerical simulations and theoretical analyses both indicate that there is a first-order phase transition in the spreading dynamics, and that a hysteresis loop emerges in the system when there is a variety of initially adopted seeds. We find an optimal community structure that maximizes spreading dynamics. We also find a rich phase diagram with a triple point that separates the no-diffusion phase from the two diffusion phases.
引用
收藏
页数:9
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