l ecture 12 c ellular a utomata 2 d iscrete t ime d
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L ECTURE 12: C ELLULAR A UTOMATA 2 / D ISCRETE -T IME D YNAMICAL S - PowerPoint PPT Presentation

15-382 C OLLECTIVE I NTELLIGENCE S18 L ECTURE 12: C ELLULAR A UTOMATA 2 / D ISCRETE -T IME D YNAMICAL S YSTEMS 4 I NSTRUCTOR : G IANNI A. D I C ARO A ZOO OF BEHAVIORS : A NY REGULARITY ? 2 C LASS 1 3 C LASS 2 Rule 2 The direction and


  1. 15-382 C OLLECTIVE I NTELLIGENCE – S18 L ECTURE 12: C ELLULAR A UTOMATA 2 / D ISCRETE -T IME D YNAMICAL S YSTEMS 4 I NSTRUCTOR : G IANNI A. D I C ARO

  2. A ZOO OF BEHAVIORS : A NY REGULARITY ? 2

  3. C LASS 1 3

  4. C LASS 2 ≪ Rule 2 The direction and location of the lines depend on the initial conditions, but the structural fact that we will have lines in a certain direction is independent from initial conditions Sierpinski gasket 4

  5. C LASS 3 Rule 184 5

  6. C LASS 4 Universal computation! 6

  7. R ULE 110 7

  8. R ULE 110: S PACE -T IME SCALES 8

  9. D EPENDENCE ON THE INITIAL STATE Dependence ~ Elaboration of initial conditions Structure does not depend but lines do No dependence  Identification of parameter of structure Trivial elaboration Strong dependence Complex elaboration,  Chaotic behaviors  Hard to predict 9

  10. D EPENDENCE ON INITIAL STATE 10

  11. L YAPOUNOV EXPONENTS Two Lyapounov exponents: measuring information propagation on initial conditions along the two directions Both 0 exponents, information doesn’t travel Positive exponents, initial information travels far away Positive exponents, going to zero 11

  12. U NIVERSAL COMPUTATION 12

  13. U NIVERSAL COMPUTATION 13

  14. L OCAL COMMUNICATIONS VS . GLOBAL BEHAVIORS 14

  15. I NVERSE PROBLEM 15

  16. R ULE 184: P ARITY PROBLEMS Why could 184 be a good candidate for parity detection problems? No single CA can solve the parity problem, but applying a sequence of elementary CAs can do it, for instance the following operator applied to a lattice of length 𝑀 : K. M. Lee, Hao Xu, and H. F. Chau , Parity problem with a cellular automaton solution , Phys. Rev. E 64 , 026702, 2001 16

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