CONNECTING DATA WITH COMPETING OPINION MODELS Oct. 31, 2014 Keith Burghardt

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CONNECTING DATA WITH
COMPETING OPINION MODELS
Keith Burghardt
with Prof. Michelle Girvan
and Prof. Bill Rand
Oct. 31, 2014
Friday, October 31, 14
OUTLINE
Introduction and background
Motivation and empirical findings
Description of our model and agreement with data
Analysis of the model
Conclusions and future work
Friday, October 31, 14
INTRODUCTION TO
OPINION DYNAMICS
Basic Idea: opinions or ideas propagate via
social interactions between individuals
Applications: adoption of languages, products,
religions, etc.
Why is important to model opinion dynamics?
Basic understanding: How do human interactions give rise to
complex social phenomena?
Practical: how can we create the largest impact, e.g. vote shares,
spread of social norms
Friday, October 31, 14
INTRO TO OPINION
DYNAMICS, CONT’D
A statistical mechanical framework for
opinion modeling:
Atoms : properties of condensed matter →
individuals : opinion dynamics
How do we understand opinion formation?
Empirical data
Intuitive models (but are they well motivated?)
Friday, October 31, 14
MODELING OPINION
DYNAMICS
Simplest model: adopt the
opinion of a randomly chosen
neighbor (Voter Model)
Often seen (e.g. Voter Model
Universality Class)
Influential
Clifford and Sudbury, Biometrika (1973)
Holley and Liggett, Ann. Prob. (1975)
Redner MAPCON (2012)
Dornic et al., Phys. Rev. Lett. (2001)
Friday, October 31, 14
TYPICAL MODEL ISSUES
Inconsistent phenomenological models
Motivation often based on results and not the
dynamics themselves
Unrealistic results (e.g., in equilibrium,
everyone has a single opinion)
Friday, October 31, 14
GOALS OF OUR MODEL
Phenomenological: capture statistical patterns
observed in data
Realistic macro-dynamics: e.g., slow convergence to
consensus/non-consensus in equilibrium
Realistic micro-dynamics: Well-motivated
mechanistic rules for the spread of ideas
Friday, October 31, 14
MOTIVATING
DATA
Top: universal scaling for a
candidate’s share of votes
Q: # candidates (opinions)
v: # voters for a candidate (opinion holders)
N: # votes (nodes)
Bottom: vote correlation
~ - log(distance)
Stubbornness (resistance to
opinion change) seems to
increases with time
Fortunato and Castellano, Phys. Rev. Lett. (2007)
Fernandez-Gracia et al, Phys. Rev. Lett (2014)
Friday, October 31, 14
UNIFYING
OBSERVATIONS WITH A
SINGLE MODEL
Our Model: Competitive Contagions with Individual
Stubbornness (CCIS Model)
Contagion-like spread of opinions (opinions are “caught” like a cold)
The longer an individual has an opinion the less likely they are to
change it (stubbornness)
Individuals occasionally re-evaluate their opinions and “recover” to the
unopinionated state
Well motivated micro-dynamics:
Contagion-like spread, stubbornness, and recovery are all in qualitative
agreement with empirical data
Friday, October 31, 14
MODEL ASSUMPTIONS
Fixed, undirected, network with N
nodes, and Q opinion states
A node i is in state {0, 1, 2, ...., Q} (0 is
the un-opinionated state)
At time t = 0, n0 nodes are in state 0, n1
with opinion 1, ... , nQ with opinion Q.
Friday, October 31, 14
MODELING DYNAMICS
ON NETWORKS
Wikipedia
Dynamics modeled
on a variety of
networks
Representative of
real social networks
(c) Lattice Network
Friday, October 31, 14
(d) “Small-World”
Network
ARE ASSUMPTIONS
REASONABLE?
Fixed number of opinions: e.g. jury verdict
(“guilty” vs. “not guilty”)
Assume a few (not necessarily all) individuals
exhibit an innate opinion preference
Candidates not well known in the beginning
Some individuals seeded with preferences, e.g. candidate
himself
Friday, October 31, 14
MODEL OVERVIEW
Convert un-opinionated
neighbor with probability
!
Adoption probability
decreases with time an
individual i has had an
infection ("i)
After "i > 1/#, an opinion
“freezes”
Opinionated (even frozen)
individuals recover at a
rate $
Friday, October 31, 14
β
Padopt
0
µ-1
τ
τi
β
β (1-τi μ)
τj
δ
No Opinion
Opinion 1
Opinion 2
β (1-τj μ)
δ
EXPLAINING
VOTE
DISTRIBUTIONS
Goal:
Fit several voter distributions with
consistent parameters
3 fitting parameters
Persuasiveness (! = 0.5)
Initial fraction with a candidate
preference (6%)
Network degree distribution
(p(k) ~ k-2.9)
All other parameters fixed
Friday, October 31, 14
Vote probability distributions, shifted by
decades (inset: original data collapse).
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Closed markers represent empirical data.
Open markers represent model results.
EXPLAINING
OBSERVATIONS:
LONG-RANGE
CORRELATIONS
Correlation of US Presidential Elections
Assume if ! (recovery) → 0,
model behaves diffusively
C(r) ~ - log(r)/log(t)
(2 dimensions)
Slow consensus!
Simulations corroborate this
behavior
Friday, October 31, 14
2000 Presidential Election
AGREEMENT WITH
SIMULATION
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Á
2D grid with rewired
connections (with no
recovery or stubbornness)
CHrL
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Rewire: small world, with long-range
correlations
A Lattice and “Small World”-type Graph
Friday, October 31, 14
ANALYTIC TREATMENT:
MEAN FIELD
APPROXIMATION
Time
Density Of
Individuals With
Opinion A
A
(t, !)
Length Of Time Since
Adopting A
(!)
Friday, October 31, 14
(t)
(t)
MEAN FIELD ANALYSIS
Mean field PDE:
[@t + @⌧ ]⇢A (t, ⌧ ) =
PA (t) ⌘
Z
1
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⇢A (t, ⌧ )d⌧
P
B6=A
k✓(1
Cyan: losses due to “recovery”
1.0
DPeq
Blue: losses due to competing opinions
Right: Difference in Q = 2 opinion
densities versus persuasiveness.
⌧ µ]⇢A (t, ⌧ )PB (t)
Difference in Opinion Densities
Versus Persuasiveness
0
Close agreement with
simulation:
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N = 105, K-regular random graph with K = 10
Friday, October 31, 14
A CLOSER LOOK AT THE
MEAN FIELD EQUATION
[@t + @⌧ ]⇢A (t, ⌧ ) =
X
⇢A (t, ⌧ )
k✓(1
⌧ µ)[1
⌧ µ]⇢A (t, ⌧ )PB (t)
B6=A
A
Cyan/Blue:
Loss/gain due to conversion to/from
Blue: contrary opinions
Cyan: the unopinionated state
(t, !)
Red: Total loss
Green: Total gain
!
-1
"
+
+
⇢A (t, 0 ) = (0 ) k[
X
PB (t)]
B6=A
[1
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X
B6=A
Friday, October 31, 14
PB (t)+
Z
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⌧ 0 µ]d⌧ 0 ]
MOTIVATION FOR A SLOW
CONSENSUS MODEL
Relatively little consensus in day-today ideas, even after many years:
Example of Consensus
1.0
GM vs. Toyota?
rA HtL
0.8
0.6
Obama vs. Romney?
Tcons
0.4
0.2
0.0
0
2000
4000
6000
8000
Long-range vote-correlations often =
model with consensus
t
Realistic models should have either
slow consensus or non-consensus.
Friday, October 31, 14
SLOW CONSENSUS
SIMULATIONS
105
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10
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101 -3
10
10-2
10-1
m
Friday, October 31, 14
Analytic treatment: assume
Voter Model-like dynamics
Ú
Û
Ú
Û
~m4.8
Ú
Û
100
Theory: Tcons ~ #2, where # is
individual “stubbornness”
DEPENDENCE ON
NETWORK SIZE
In the mean field limit,
consensus time scales as:
Tcons ⇠
Tcons
103
‡
102
Ù
Ù Ù Ù
Tcons ⇠ 1/N
Ù
8000
105
N
10
Ê
Tcons
0
104
2
2)/(↵ 1)
‡
‡ ‡
‡ ‡
Ù
Ê
Ù Ù
‡
Ê
Ê
Ù
‡
Ù Ù Ê Ê Ê Ê Ê Ê
Ù Ê
Ê
1.0
Ù Ê
Ê
Tcons
0.5
/µ)2
Complete graph:
Friday, October 31, 14
‡ ‡
‡
‡
101
For scale-free networks:
Tcons ⇠ N 2(↵
‡
0.0
N
hk 2 i(
a
Ê 2.1
Ù 2.5
‡ 2.9
Ê
Ê
Ê
101
Ê
Ê
Ê
100
102
103
N
104
IMPLICATIONS OF OUR MODEL
Checking model
assumption: does
stubbornness increase in
time?
10
Friday, October 31, 14
Ï
-1
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Ï
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ÊÊ
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ÚÚÏÚÏ
-2
10
ÚÏÚÏÚ
Ú ÏÏ ÊÊ
ÏÚÚ
ÊÏÚ
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ÏÏÚ
Ê
Ê
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Ú
Ê
Ê
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10-3 Ú ÏÏ Ê
ÚÚ
ÊÊ
ÊÊ
10-4 Ï
10-2
Brand share probability should
follow a distribution alike to the
right figure
Q = 10
Q = 20
Q = 30
Ê
PHv,Q,NL
Checking model
prediction: if stubbornness
= brand loyalty:
100
Rescaled Brand-share Probability Distribution
10-1
100
101
v QêN
v: Number of items sold
N: total number of items
Q: Number of brands
102
SUMMARY OF RESULTS
We created a minimal model with:
Strong agreement to empirical data
Realistic macrodynamics
Well motivated microdynamics
Found analytically tractable results on dynamics and
consensus
Presented ways to further corroborate our model
Friday, October 31, 14
ADDING GREATER
REALISM
Opinion Difference Versus Random Flip Rate
1.0
Random opinion
flipping
Potentially in the
Ising Model
Universality Class
Friday, October 31, 14
0.8
DPeq
3(!) critical points
4.00 ¥ 102
8.00 ¥ 102
1.60 ¥ 103
3.20 ¥ 103
6.40 ¥ 103
1.28 ¥ 104
2.56 ¥ 104
5.12 ¥ 104
0.6
0.4
0.2
0.0
0.00
0.02
0.04 0.06
Flip Rate
0.08
0.10
OPEN QUESTIONS
What is the relation between model time-steps and
the real world?
How can we determine the microdynamics, versus
aggregate macrodynamic data?
How does stubbornness evolve?
Friday, October 31, 14
Thank You
Questions?
Friday, October 31, 14
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