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

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

Dynamic percolation, exceptional times, and

harmonic analysis of boolean functions

Oded Schrammjoint w/ Jeff Steif

Page 2: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Percolation

Page 3: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Dynamic Percolation

Page 4: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

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?

Page 5: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

• Any infinite graph G has a pc:

• 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…

Häggström, Peres, Steif (1997)

Page 6: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

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.

Page 7: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

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].

Page 8: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

2nd moment argument

We show that

Then use Cauchy-Schwarz:

Page 9: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

2nd moment spelled out

Consequently, enough to show

Page 10: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Interested in expressions of the form

Where is the configuration at time

t, and f is a function of a static configuration.

Rewrite

where

Page 11: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Understanding Tt

Set

Then

Page 12: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Set

Then

Write

Page 13: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif
Page 14: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Theorem (BKS): When fn 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

Page 15: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Need more quantitative

Conjectured (BKS):

with

We (SS) prove this (for Z2 and for the triangular grid).

Page 16: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

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.

?

Page 17: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

The of percolation

Not optimal, (simulations) [LSW,Sm][PSSW]

Page 18: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Annulus case δ

Page 19: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Annulus case δ

The for the algorithm calculating

is approximately

get to approx radius r

visit a particular hex

Page 20: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Putting it together

Etc...

Page 21: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

What about Z2 ?

• The argument almost applies to Z2

Need

2. Improve (better algorithm)

1. Have

3. Improve Fourier theorem

4. Calculate exponents for Z2

Page 22: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

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:

Page 23: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Next

• Proof of Fourier estimate

• Further results

• Open problems

• End

Page 24: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

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

Page 25: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Fourier coefficients change under algorithm

When algorithm examines bit :

Page 26: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Proof of Fourier Thm

Set

Page 27: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

QED

Page 28: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Further results

Never 2 infinite clusters.

Page 29: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Wedges

Page 30: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Wedges

• Exceptional times with k different infinite clusters if

• HD:

• None if

Page 31: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Cones

glue

Page 32: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Cones

• Exceptional times with k>1 different infinite clusters if

• HD:

• None if

Page 33: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

Open problems

• Improve estimate for

• Improve Fourier Theorem

• Percolation Fourier coefficients

• Settle

• Correct Hausdorff dimension?

• Space-time scaling limit

Page 34: Dynamic percolation, exceptional times, and harmonic analysis of boolean functions Oded Schramm joint w/ Jeff Steif

The End