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Physical Considerations on the Schelling model of Social Segregation Sergio Rica Universidad Adolfo Ibez In collaboration with N. Goles-Domic and E. Goles Phys Rev E 83, 056111 (2011) On the occasion of the 60th birthday of Prof. Eric


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Physical Considerations on the Schelling model of Social Segregation

Sergio Rica Universidad Adolfo Ibáñez In collaboration with N. Goles-Domic and E. Goles Phys Rev E 83, 056111 (2011)

On the occasion of the 60th birthday of Prof. Eric Goles

Valparaíso, nov 2011

Supported by grant COSTUME, ANR SYSCOM (France)

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Plan

Introduction The Schelling Model Qualitative behavior Quantitative behavior Discussion

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The Model of Segregation by Shelling

Lattice {i,k}

xk

xk

xk

xk = ±1

State

Vicinity Tolerance threshold

Thomas C. Schelling (1969 - 1972)

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Happiness threshold

An individual is unhappy if there are more than individuals of the other type.

θ

  • eg. in a vicinity
  • f 8 neighbors

and if then :

θ = 5

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The rule

At each step, one lists the unhappy individuals of both species, and then randomly one exchanges two individuals of

  • pposite specie.

R e m a r k : t h e n u m b e r o f individuals of each specie (N+ & N- ) are conserved.

  • i,k

xik = N+ − N− = Cte

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θ = 5

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Phase diagram

  • 4

3 2 5 6 25% 50%

finite time evolution infinite time evolution

12.5% 7 φ = N+ N+ + N−

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Comments

A tendency of segregation. A tendency of a diminution of the interfaces But! there is a strong frustration. A length scale ?

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256 x 256

128 x 128

32 x 32 64 x 64

512 x 512 Length scale for θ = 5

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Case of 44 neighbors

8 neighbors

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Case of 68 neighbors

8 neighbors

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Summary

8 neighbors 68 neighbors 44 neighbors

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Quantitative behavior

E[{x}] = −1 2

N

  • k=1

xk

  • i∈Vk

xi

θ = 5

decreases strictly during the evolution. Moreover, ∆Ekl ≤ 4 (wkl + 8 − 2θ)

wkl ≤ 1

where For 8 neighbors and, if and higher, then the “energy"

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Geometrical interpretation

E[{x}] = −1 2

N

  • k=1
  • i∈Vk

1 + 1 2

N

  • k=1
  • i∈Vk

(1 − xkxi) = −1 28N + 1 2

N

  • k=1
  • i∈Vk

(1 − xkxi) E = −4N + 2 ×

  • 3
  • edges −
  • corners
  • = −4N + 2 × (3 × perimeter − Nb. of corners),
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Few Consequences

Because the energy is bounded

  • 4 N ≤ E ≤ 4 N the dynamics is
  • f finite time for and

higher. For the dynamics continues indefinitely The case may posses a complex dynamics The energy ground state.

θ = 5 θ ≤ 3 θ = 4

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Phase diagram

  • 4

3 2 5 6 25% 50%

finite time evolution infinite time evolution

12.5% 7 φ = N+ N+ + N−

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E vs time

E/N t [10 units ]

3

=5 =4 =3 =2 =6

GSE

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E vs time

E/N t [10 units ]

3

=2

GSE

=3 =4 =5

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Discussion

Var i a nt s o n t h e m o d e l a n d g en eralizatio ns (g rap hs, no n uniform tolerance, various states, protocols...) Q2R Segregation in higher dimensions ?

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Segregation in 3D