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Dynamic percolation, exceptional times, and harmonic analysis of boolean functions

Dynamic percolation, exceptional times, and harmonic analysis of boolean functions. Oded Schramm. joint w/ Jeff Steif. Percolation. Dynamic Percolation. Infinite clusters?. Harris (1960): There is no infinite cluster Kesten (1980): There is if we increase p. For static percolation:.

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Dynamic percolation, exceptional times, and harmonic analysis of boolean functions

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  1. Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

  2. Percolation

  3. Dynamic Percolation

  4. Infinite clusters? • Harris (1960): There is no infinite cluster • Kesten (1980): There is if we increase p For static percolation: For dynamic percolation: • At most times there is no infinite cluster • Can there be exceptional times?

  5. Any infinite graph G has a pc: Häggström, Peres, Steif (1997) • Above pc: • Below pc: • The latter at pc for Zd, d>18. • Some (non reg) trees with exceptional times. • Much about dynamic percolation on trees…

  6. Exceptional times exist Theorem (SS): The triangular grid has exceptional times at pc. This is the only transitive graph for which it is known that there are exceptional times at pc.

  7. Proof idea 0: get to distance R • Set • We show Namely, with positive probability the cluster of the origin is unbounded for t in [0,1].

  8. 2nd moment argument We show that Then use Cauchy-Schwarz:

  9. 2nd moment spelled out Consequently, enough to show

  10. Interested in expressions of the form Where is the configuration at time t, and f is a function of a static configuration. Rewrite where

  11. Understanding Tt Set Then

  12. Set Then Write

  13. Noise sensitivity Theorem (BKS): When fnis the indicator function for crossing an n x n square in percolation, for all positive t Equivalently, for all t>0 fixed Equivalently, for all k>0 fixed

  14. Need more quantitative Conjectured (BKS): with We (SS) prove this (for Z2 and for the triangular grid).

  15. Estimating the Fourier weights Theorem (SS): Suppose that there is a randomized algorithm for calculating f that examines each bit with probability at most . Then ? Probably not tight.

  16. The  of percolation [LSW,Sm] [PSSW] Not optimal, (simulations)

  17. Annulus case δ

  18. Annulus case δ The  for the algorithm calculating is approximately get to approx radius r visit a particular hex

  19. Putting it together Etc...

  20. 1. Have Need 3. Improve Fourier theorem What about Z2 ? • The argument almost applies to Z2 2. Improve  (better algorithm) 4. Calculate exponents for Z2

  21. How small can  be BSW: • Example with • Monotone example with • These are balanced • Best possible, up to the log terms • The monotone example shows that the Fourier inequality is sharp at k=1.

  22. Next • Proof of Fourier estimate • Further results • Open problems • End

  23. Theorem (SS): Suppose that there is a randomized algorithm for calculating f that examines each bit with probability at most δ. Then

  24. Fourier coefficients change under algorithm When algorithm examines bit :

  25. Proof of Fourier Thm Set

  26. QED

  27. Further results Never 2 infinite clusters.

  28. Wedges

  29. Wedges • Exceptional times with k different infinite clusters if • None if • HD:

  30. Cones glue

  31. Cones • Exceptional times with k>1 different infinite clusters if • None if • HD:

  32. Open problems • Improve estimate for • Improve Fourier Theorem • Percolation Fourier coefficients • Settle • Correct Hausdorff dimension? • Space-time scaling limit

  33. The End

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