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

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Presentation on theme: "Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif."— Presentation transcript:

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 p c : Above p c : Below p c : The latter at p c for Z d, d>18. Some (non reg) trees with exceptional times. Much about dynamic percolation on trees… Häggström, Peres, Steif (1997)

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

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

9 2 nd 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 T t Set Then

12 Set Then Write

13

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

15 Need more quantitative Conjectured (BKS): with We (SS) prove this (for Z 2 and for the triangular grid).

16 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. ?

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

18 Annulus case δ

19 The  for the algorithm calculating is approximately get to approx radius r visit a particular hex

20 Putting it together Etc...

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

22 Interface

23 How small can  be 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. BSW:

24 Next Proof of Fourier estimate Further results Open problems End

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

26 Fourier coefficients change under algorithm When algorithm examines bit :

27 Proof of Fourier Thm Set

28 QED

29 Further results Never 2 infinite clusters.

30 Wedges

31 Exceptional times with k different infinite clusters if HD: None if

32 Cones glue

33 Cones Exceptional times with k>1 different infinite clusters if HD: None if

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

35 The End


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