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Consensus and Polarization in a Three-State

Constrained Voter Model

Mauro Mobilia

Department of Applied Mathematics University of Leeds

“The Unexpected Conference”, Paris 14-16/11/2011

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Outline

Talk based on the paper: EPL (Europhysics Letters)95, 50002 (2011)

[arXiv:1104.5147]

Emergence of diversity is a complex problem in life and behavioural sciences: main features to be incorporated in basic models?

Basic and unifying principles of evolutionary dynamics The 2-state voter model

The 3-species constrained voter model The model and solution method The exit/fixation probabilities The mean exit/fixation times

Conclusion

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Basic principles of evolutionary dynamics

Key questions:how is diversity maintained?

Opinion dynamics context: when is there consensus / cultural diversity?

Basic and unifying principles for modelling evolutionary dynamics:

Dynamics proceeds by imitation

Selection: successful “opinions” spread at the expense of the others

Population is finite and there are demographic fluctuations Mutations: spontaneously switch from an opinion to another Migration: opinions/individuals spread in space (“islands”, “patches”,...)

These principles transcend biology and behavioural science (opinion dynamics, evolutionary games, genetics, ecology, ...).

Paradigmatic opinion dynamics model:the voter model(related to

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2-state Voter Model

Voter Model (Liggett 1985, Galam 1990): Basic/paradigmatic

two-state model where individuals are either in+1 (↑) or−1 (↓)

opinion state.Dynamics: at each time step an individual adopts the

opinion state of a random neighbour

Main properties forNvoters on a complete graph, with an initial

fractionx of+1:

Consensus is always reached

Probability to reach+1 and−1 consensus isx and 1−x, resp. Mean time to attain consensus isT ∼N

2-state VM cannot explain the emergence of cultural diversity Axelrod’97, Deffuant’00, Weisbuch’02: competition between

consensus&incompatibility⇒possible route to cultural diversity (?)

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The 3-species constrained voter model

Nindividuals of 3 species.A’s (leftists) andB’s (rightists) are

incompatible(don’t interact), but interact withcentristsC’s (|q| ≤1)

AB→AB; AC →AA rate: 1+q 2 , AC→CC rate: 1−q 2 BC →BB rate: 1+q 2 , BC→CC rate: 1−q 2

4 possible outcomes: consensus withA,BorC, or frozen mixture of AandB(polarization)⇒Probability and mean time for each of these events starting with densitiesx,y,z=1−x−y ofA,B,C?

q>0: bias towards polarization(extremisms), with absorbing linex+y=1 q<0: bias towardscentrism (appeasement)

q=0: driven by fluctuations

[Vazquez & Rednerin

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3-species constrained voter model: Mean-field

Mean field picture: all fluctuations are neglected (assume thatN=∞)

Deterministic dynamics in terms of rate equations:

d dta = qa(1−a−b), d dtb=qb(1−a−b) a(t) = xe qt 1−(x+y)(1−eqt), b(t) = yeqt 1−(x+y)(1−eqt)

Ratioa/b=x/y is conserved. 3 absorbing fixed points,

(a,b,c)∈ {A = (1,0,0),B= (0,1,0),C = (0,0,1)}+(polarization) line of fixed pointsA B= (a,1−a,0), with 0<a<1

Whenq>0: a→ x x+y,b→ y x+y,c→0 (polarization) Whenq<0: a→0,b→0,c→1 (centrism)

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3-species constrained VM: Individual-based approach

Finite population (N<∞): fluctuations alter the mean field

predictions.Polarization is likely whenq>0, but still probability to reach a consensus. (The opposite whenq<0)

Stochastic formulationof a finite and well-mixed (“complete graph”) population

Starting from(x,y), probabilityPA B(x,y)that final state is a frozen

mixture of extremists obeys the backward master equation (ME)

(Tx++Tx−+Ty++Ty−)PA B(x,y) =

Tx−PA B(x−δ,y) +Tx+PA B(x+δ,y)

+ Ty−PA B(x,y−δ) +Ty+PA B(x,y+δ) (1)

+ boundary conditions. WithT±

ξ ≡(1±q)ξ(1−x−y)/2,ξ ∈(x,y)

andδ=N−1

Analytical progress: expand the ME to 2nd order inδ →

Fokker-Planck equation.Analogy with models of population genetics

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3-species voter model: Mathematical treatment (I)

By Taylor expansion of the ME (1):

LbFP(x,y)PA B(x,y) =n2s[x∂x+y∂y] +x∂x2+y∂y2

o

PA B(x,y) =0, (2)

withsNqandPA B(x,0) =PA B(0,y) =0 andPA B(x,1−x) =1.

Equation isseparable(√x=ρcosθ,√y=ρsinθ):

PA B=∑ncnRn(ρ)un(θ)sin(2θ), yielding ρ2d 2R n dρ2 +ρ dRn dρ [4sρ 21] λnRn=0 d2un dθ2 − 3 4 1 sin2θ + 1 cos2θ un+ (1+λn)un=0 BC:PA B(ρ=0,θ) =0 andPA B(ρ=1,θ) =1⇒λn=4(n+1)(n+2) PA B(x,y) =2 r xy x+ye s(1−x−y) ∞

nodd 2n+1 n(n+1) I n+1/2(s(x+y)) In+1/2(s) Pn1 xy x+y

In’s andPn1’s: Modified Bessel functions & associated Legendre

Polynomials.

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Exit probabilities when

s

=

Nq

>

0

Whens=N|q| 1: drift dominates over diffusion⇒mean field

Whens1: drift negligible⇒like in JPA37, 8479 (2004))

Effective (interesting) competition arises whens=Nq=O(1)

Top: Exit probabilities fors>0 as

functions ofx (forN=200,s=4,

i.e.q=0.02):

PA (),PB (4),PC ();PA B (◦)

Solid line: analytical sol. of (2)

Bottom: same as above, but with

x =2y.

Inset:final densities of speciesA

(×) andB(+) as functions of

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Exit probabilities when

s

<

0

Top: as before, withs=−4

Comparison with analytics: Solid: solution of (2) Dashed:

PA B≈1−PC =e2|s|(x+y)−1 e2|s|1

Bottom: as above, but withx =2y.

Inset:stationary density ofA(×)

as function ofx =2y compared

with analytics

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3-species voter model: Mathematical treatment (II)

The unconditional mean exit/fixation time (MET)τto reachanyof the

system’s absorbing states obeys the backward Fokker-Planck

equation with BCτ(1,0) =τ(0,1) =τ(0,0) =τ(a,1−a) =0. With

w≡x+y: LbFP(w) = w(1−w) N 2s d dw+ d2 dw2 LbFP(w)τ(w) =−1, with τ(0) =τ(1) =0⇒ (3)

Useful mapping with a population genetics model (sis “selection

strength”)

The unconditional METτ=τ(x+y):

is a function of initial density of extremists (x+y)

scales linearly withN

symmetry: invariant under(s,x+y)→(−s,1−x−y)⇒

τ(x+y) =Nfτ(s,x+y) =Nfτ(−s,1−x−y)

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Unconditional & Conditional Mean Exit Times

TheconditionalMETτS, to reach the specific absorbing state

S ∈(A,B,C,A B)obeys:

LbFP(x,y)[PS(x,y)τS(x,y)] =−PS(x,y)

(+BC’s),

where thePS(x,y)’s are exit/fixation probabilities

AllτS’s are found to scale linearly withN

TheτS’s do not depend on the sign ofs (more noisy when s<0)

The extremists’ METs,τA andτB, are always the longest METs

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Mean Exit Times

Normalized unconditional MET

τ/N(×)compared with sol. of (3)

(solid)

Normalized conditional METs

τA/N()

τB/N(•) τC/N()

τA B/N(◦).

N=200,x=y,s=4 (top) and

s=−4 (bottom). Average is over

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Outlook & Conclusion

Understanding the origin and maintenance of diversity in evolutionary dynamics

Seek for consensus & incompatibility: relevant ingredients for cultural diversity in opinion dynamics(?)

The 3-state constrained voter model is mathematically amenable: Possible outcomes: consensus with extremists/centrists, or polarization of extremism (“leftists” and “rightists” coexist) Bias (∼selection)→nonlinearity. Finite population→noise Small bias (q∼N−1, “weak selection”): subtle competition between drift and fluctuations

How relevant all of this is?

Realistic ingredients: mutations, dispersal, spatial structure

Validation a variant of the model using real data?

References

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