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A tight race between deterministic and stochastic dynamics of - - PowerPoint PPT Presentation

A tight race between deterministic and stochastic dynamics of RPS-model Qian Yang Supervisors: Prof. Jonathan Dawes & Dr. Tim Rogers University of Bath Email: Q.Yang2@bath.ac.uk July 5, 2016 . . . . . . . . . . . . . . . .


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A tight race between deterministic and stochastic dynamics of RPS-model

Qian Yang

Supervisors: Prof. Jonathan Dawes & Dr. Tim Rogers University of Bath Email: Q.Yang2@bath.ac.uk

July 5, 2016

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 1 / 16

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Overview

1

Motivation

2

RPS-Model 2.1 Rock-Paper-Scissors - It’s just a GAME. 2.2 ODEs and simulations for RPS-model - We found a RACE! 2.3 Three regions of average period of these cycles - WHO WINS?

3

Summary

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 2 / 16

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  • 1. Motivation

Cyclic Dominance (Rock-Paper-Scissors)–

1 widely exists in nature, eg. Biology, Chemistry 2 describes the interactions between species Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 3 / 16

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  • 1. Motivation

Analysis Method –

1 Deterministic: Continuous and

infinite.

2 Stochastic: Discrete and finite

Main work –

1 Agreement and disagreement of

RPS-model with the two methods.

2 Noise slows down the evolution of

cyclic dominance.

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 4 / 16

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2.1 Rock-Paper-Scissors Game

RPS simplest model

B(Paper) A(Rock) C(Scissors) x y : x beats y

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 5 / 16

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2.1 Rock-Paper-Scissors Game

RPS simplest model

B(Paper) A(Rock) C(Scissors) x y : x beats y

Payoff matrix P = A B C A B C   1 −1 −1 1 1 −1  

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 5 / 16

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2.1 Rock-Paper-Scissors Game

RPS simplest model

B(Paper) A(Rock) C(Scissors) x y : x beats y

Payoff matrix P = A B C A B C   1 −1 −1 1 1 −1   Differential equations for deterministic study

˙ a = a(c − b), ˙ b = b(a − c), ˙ c = c(b − a), and a(t) + b(t) + c(t) = 1.

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 5 / 16

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2.1 Rock-Paper-Scissors Game

RPS simplest model

B(Paper) A(Rock) C(Scissors) x y : x beats y

Payoff matrix P = A B C A B C   1 −1 −1 1 1 −1   Differential equations for deterministic study

˙ a = a(c − b), ˙ b = b(a − c), ˙ c = c(b − a), and a(t) + b(t) + c(t) = 1.

Chemical reactions for stochastic simulation

A + B

1

− → B + B, B + C

1

− → C + C, C + A

1

− → A + A, and A + B + C = N, N is fixed.

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 5 / 16

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2.1 Rock-Paper-Scissors Game

Update the simplest RPS-model RPS-model with mutation and unbalanced payoff

B(Paper) A(Rock) C(Scissors) x y : x beats y x y : x mutates into y

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 6 / 16

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2.1 Rock-Paper-Scissors Game

Update the simplest RPS-model RPS-model with mutation and unbalanced payoff

B(Paper) A(Rock) C(Scissors) x y : x beats y x y : x mutates into y

Payoff matrix P = A B C A B C   1 −β − 1 −β − 1 1 1 −β − 1   + Mutations

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 6 / 16

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2.1 Rock-Paper-Scissors Game

Update the simplest RPS-model Ordinary Differential Equations ˙ a = a[c − (1 + β)b + β(ab + bc + ac)] + µ(b + c − 2a), ˙ b = b[a − (1 + β)c + β(ab + bc + ac)] + µ(c + a − 2b), ˙ c = c[b − (1 + β)a + β(ab + bc + ac)] + µ(a + b − 2c). with β > 0 and µ > 0, µ is mutation rate.

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 7 / 16

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2.1 Rock-Paper-Scissors Game

Update the simplest RPS-model Ordinary Differential Equations ˙ a = a[c − (1 + β)b + β(ab + bc + ac)] + µ(b + c − 2a), ˙ b = b[a − (1 + β)c + β(ab + bc + ac)] + µ(c + a − 2b), ˙ c = c[b − (1 + β)a + β(ab + bc + ac)] + µ(a + b − 2c). with β > 0 and µ > 0, µ is mutation rate. Chemical reactions for stochastic simulations

A + B

1

− → B + B, B + C

1

− →C + C, C + A

1

− → A + A, A + B + B

β

− → B + B + B, A

µ

− → B, A

µ

− → C, A + A + C

β

− → A + A + A, B

µ

− → C, B

µ

− → A, B + C + C

β

− → C + C + C, C

µ

− → A, C

µ

− → B.

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 7 / 16

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2.2 Analysis of ODEs

Jacobian Matrix of ODEs

1 The only interior equilibrium:

x∗ = (a∗, b∗, c∗) = (1/3, 1/3, 1/3)

2 Jacobian matrix around the equilibrium

J∗ = (− 1

3 − 3µ

− 2

3 − 1 3β 2 3 + 1 3β 1 3 + 1 3β − 3µ

)

3 The critical value of µ:

µc = β 18.

4 When µ < µc, Hopf bifurcation happens. Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 8 / 16

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2.2 Numerical solution of ODEs

Formation of a robust cycle - limit cycle Figure: β = 1

2, µ = 1 216 < µc = 1 36, y1 = a + 1 2b, y2 = √ 3 2 b.

0.2 0.4 0.6 0.8 1 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9

The coordinates transformation makes the flow spiraling outwards visible.

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 9 / 16

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2.2 Stochasitic simulations

Comparison with numerical solution to ODEs Figure: β = 1

2, µ = 1

  • 216. N is total of individuals in simulation.

Behave differently. SSA - Stochastic Simulation Algorithm. Size N controls the level of randomness.

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 10 / 16

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2.2 Quasi-periodic cycles

Average period of these quasi-periodic cycles An interesting comparison: There is a RACE between stochastic dynamic and deterministic dynamic!

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 11 / 16

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2.3 Region I - the right part

Determinsitic dynamic governs the game Compose local and global map:

global map local map

(0,0,1) (1,0,0) (0,1,0)

TODE ∝ − ln µ is proved theoretically.

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 12 / 16

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2.3 Region III - the left part

Stochastic dynamic prevails the opponent The cycle in this region looks like: It is a 1-D death-birth process. When µ ≪

1 N ln N , TSSA ∝ 1 Nµ.

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 13 / 16

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2.3 Region II - the middle part

A tight race between the two dynamics Explanation: the idea of asymptotic phase (the picture, cited from J.

  • M. Newby) and SDE.

When µ ∼

1 N ln N , TSDE ≈ −3 ln µ + C 3 Nµ.

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 14 / 16

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  • 3. Summary - Three regions

Region Winner Methods Figure Region I

1 N ln N ≪ µ < µc

Deterministic TODE ∝ − ln µ composition of local and global maps

global map local map

(0,0,1) (1,0,0) (0,1,0)

Region II µ ∼

1 N ln N

Even TSDE ≈ −3 ln µ + C

3 Nµ

asymptotic phase and SDE Region III 0 < µ ≪

1 N ln N

Stochastic TSSA ∝

1 Nµ

Markov Chain

Table: Different result of the race in different region.

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 15 / 16

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  • 3. Summary - Final comparison

A tight race between the two dynamics Summarise three theoretical analysis, and draw the following figure:

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 16 / 16

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  • 3. Summary - Final comparison

A tight race between the two dynamics Summarise three theoretical analysis, and draw the following figure: Finally, the result of the match is revealed. Thank you for your attention!

Qian Yang (Uni. of Bath) Different dynamics in cyclic dominance July 5, 2016 16 / 16