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Physical Mechanism Underlying Opinion Spreading

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1 Physical Mechanism Underlying Opinion Spreading
Jia Shao Shlomo Havlin, H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, (2009).

2 Questions How can we understand, and model the coexistence of two mutually exclusive opinions? Is there a simple physical mechanism underlying the spread of mutually exclusive opinions?

3 Motivation Coexistence of two (or more) mutual exclusive opinions are commonly seen social phenomena. Example: US presidential elections Community support is essential for a small population to hold their belief. Example: the Amish people Existing opinion models fail to demonstrate both.

4 What do we do? We propose a new opinion model based on local configuration of opinions (community support), which shows the coexistence of two opinions. If we increase the concentration of minority opinion, people holding the minority opinion show a “phase transition” from small isolated clusters to large spanning clusters. This phase transition can be mapped to a physical process of water spreading in the layer of oil.

5 Evolution of mutually exclusive opinions
: =2:3 Time 0 : =3:4 Time 1 stable state (no one in local minority opinion) Time 2

6 A. Opinion spread for initially
: =2:3 stable state : =1:4

7 B. Opinion spread for initially
: =1:1 stable state : =1:1

8 “Phase Transition” on square lattice
B largest size of the second largest cluster ×100 A critical initial fraction fc=0.5

9 2 classes of network: differ in degree k distribution
Poisson distribution: Power-law distribution: (i) Erdős-Rényi (ii) scale-free Edges connect randomly Preferential Attachment Log P(k) Log k

10 “Phase Transition” for both classes of network
fc≈0.46 fc≈0.30 (b) scale-free (a) Erdős-Rényi Q1: At fc , what is the distribution of cluster size “s”? Q2: What is the average distance “r” between nodes belonging to the same cluster?

11 Invasion Percolation A: Injection Point
Example: Inject water into layer containing oil Invasion percolation describes the evolution of the front between two immiscible liquids in a random medium when one liquid is displaced by injection of the other. Trapped region will not be invaded. A: Injection Point D. Wilkinson and J. F. Willemsen, J. Phys. A 16, 3365 (1983).

12 Invasion Percolation Fractal dimension: 1.84 s ~r1.84
Trapped Region of size s P(s) ~ s-1.89 S Fractal dimension: 1.84 s ~r1.84 S. Schwarzer et al., Phys. Rev. E. 59, 3262 (1999).

13 Clusters formed by minority opinion at fc
Cumulative distribution function P(s’>s) ~ s-0.89 r/s(1/1.84) Const. s ~ r1.84 PDF P(s) ~ s-1.89 Conclusion: “Phase transition” of opinion model belongs to the same universality class of invasion percolation.

14 Summary Proposed an opinion model showing coexistence of two opinions.
The opinion model shows phase transition at fc. Linked the opinion model with an oil-field-inspired physics problem, “invasion percolation”.

15 Thank you!


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