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Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanle y Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701 (2
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Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

Dec 20, 2015

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Page 1: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

Physical Mechanism Underlying Opinion Spreading

Jia Shao

Advisor: H. Eugene Stanley

J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701 (2009).

Page 2: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

Questions

• How do different opinions influence each other in human society?

• Why minority opinion can persistently exist?

Page 3: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

Motivation• Public opinion is important.• Simulation of opinion

formation is a challenging task, requiring reliable information on human interaction networks.

• There is a gap between existing models and empirical findings on opinion formation.

Instead of using individual level network, we propose a community level network to study opinion dynamics.

US presidential elections

Page 4: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

Outline

• Part I: Empirical findings from presidential election

• Part II: Invasion Percolation

• Part III: We propose a dynamic opinion model which can explain the empirical findings

Page 5: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

2008 Presidential ElectionPart I

fDem

fT=0.5

fT=0.3

fT=0.8

We study counties with f>fT

http://www-personal.umich.edu/~mejn/election/2008/

Page 6: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

Counties in southern New EnglandPart I

Page 7: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

Counties in southern New EnglandPart I

Page 8: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

Counties in southern New EnglandPart I

Barnstable f=55%Polymouth f=54%Norfolk f=54%Worcester f=57%Fairfield f=52%Litchfield f=47%Windham f=53%Kent f=56%

Vote for Obama

Page 9: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

Counties in southern New EnglandPart I

County network of f>fT=0.6

Number of counties:17Size of largest cluster: 10

Page 10: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

County Network of ObamaPart I

Counties of fObama>fT

50% decrease

Page 11: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

County Network of McCainPart I

Counties of fMcCain>fT

30% decrease

Page 12: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

Clusters formed by counties when fT=fc

Fractal dimension: dl=1.56 =1.86

The phase transition in county network is different from randomized county network.

Part I

County network

Diameter

Clu

ster

Siz

e

Page 13: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

• The real life county election network demonstrates a percolation-like phase transition at fT=fc.

• This phase transition is different from random percolation.

What class of percolation does this phase transition belong to?

Page 14: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

Invasion Percolation

• 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.

Example: Inject water into earth layer containing oil

A: Injection Point

D. Wilkinson and J. F. Willemsen, J. Phys. A 16, 3365 (1983).

Part II

P. G. de Gennes and E. Guyon, J. Mech. 17, 403(1978).

Page 15: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

Invasion PercolationTrapped Region of size s P(s) ~ s-1.89

Fractal dimension: 1.51 s ~l1.51

S

S. Schwarzer et al., Phys. Rev. E. 59, 3262 (1999).

Part II

Page 16: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

• The phase transition of the county election network belongs to the same universality of invasion percolation.

• Why invasion percolation?

• How can we simulate the dynamic process of opinion formation?

Page 17: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

Evolution of mutually exclusive opinions

Time 0

Time 1

Time 2

: =2:3

: =3:4

stable state(no one in local minority opinion)

Page 18: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

A. Opinion spread for initially : =2:3

stable state : =1:4

Page 19: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

B. Opinion spread for initially: =1:1

stable state : =1:1

Page 20: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

“Phase Transition” on square lattice

critical initial fraction fc=0.5

size of the second largest cluster ×100

Phase 1 Phase 2

A

B

larg

est

Page 21: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

2 classes of network: differ in degree k distribution

Poisson distribution: Power-law distribution:

P(k

)

k

Poisson distribution

Scale Free

Log(

P(k

))Log(k)

Power-lawdistribution

Edges connect randomly Preferential Attachment

(ii) scale-free (i) Erdős-Rényi

( ) ~ exp( )!

ktP k t

k ( ) ~P k k

µ Log

P(k

)Log k

µ µ

Page 22: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

“Phase Transition” for both classes of network

fc≈0.46

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?

(a) Erdős-Rényi (b) scale-free

fc≈0.30

µ

Page 23: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

Clusters formed by minority opinion at fc

Cumulative distribution function P(s’>s) ~ s-0.89

PDF P(s) ~ s-1.89

r/s(1/1.84) Const.

s ~ r1.84

Conclusion: “Phase transition” of opinion model belongs to the same universality class of invasion percolation.

r

Page 24: Physical Mechanism Underlying Opinion Spreading Jia Shao Advisor: H. Eugene Stanley J. Shao, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 103, 018701.

Summary

• There exists a phase transition in the county election network when changing fT.

• The phase transition of county network can be mapped to oil-field-inspired physics problem, “invasion percolation”.

• We propose a network model which can explain the empirical findings.