A particle representation for the heat equation solution - PowerPoint PPT Presentation

1 / 26
About This Presentation
Title:

A particle representation for the heat equation solution

Description:

A particle representation for the heat equation solution – PowerPoint PPT presentation

Number of Views:67
Avg rating:3.0/5.0
Slides: 27
Provided by: mathe190
Category:

less

Transcript and Presenter's Notes

Title: A particle representation for the heat equation solution


1
A particle representation for the heat equation
solution
  • Krzysztof Burdzy
  • University of Washington

2
Fleming-Viot model
N population size (constant in time )
ecological niche carrying capacity
Free space Population distribution converges to a
fractal structure
Let N go to infinity.
Bounded domain Population distribution converges
to a density heat equation solution
3
Competing species
4
Selected references
  • B, Holyst, Ingerman, March (1996)
  • B, Holyst, March (2000)
  • B, Quastel (2007)
  • Grigorescu, Kang (2004, 2006, 2006)

5
Multiple populations
Minimization of the Renyi entropy production in
the space-partitioning process Cybulski, Babin,
and Holyst, Phys. Rev. E 71, 046130 (2005)
6
The stationary distribution
- first Dirichlet eigenvalue in k-th region
Conjecture 1 The stationary distribution
minimizes
Bucur, Buttazzo and Henrot Existence results for
some optimal partition problems Adv. Math. Sci.
Appl. 8 (1998) 571579 Conti, Terracini and
Verzini On a class of optimal partition
problems related to the Fucik spectrum and to the
monotonicity formulae Calc. Var. 22, 4572
(2005)
Conjecture 2 The honeycomb pattern minimizes
Special thanks to Luis Caffarelli!
7
The stationary distribution (2)
()
B, Holyst, Ingerman and March Configurational
transition in a Fleming-Viot-type model and
probabilistic interpretation of Laplacian
eigenfunctions J. Phys. A 29, 1996, 2633-2642
Conjecture 3 The critical ratio r for () and
m populations satisfies
8
Rigorous results one population
Theorem (B, Holyst, March, 2000) Suppose that the
individual trajectories are independent Brownian
motions. Then
9
Idea of the proof
A parabolic function (harmonic in space-time)
A martingale plus a process with positive jumps
10
One population convergence to the heat equation
solution
  • population size
  • individual particle mass
  • empirical density at time
  • individual trajectories follow Brownian motions

Theorem (B, Holyst, March, 2000) If
then
where is the normalized heat
equation solution with
11
One population convergence of stationary
distributions
  • population size
  • individual particle mass
  • empirical density at time
  • individual trajectories follow Brownian motions

Theorem (B, Holyst, March, 2000) The process
has a stationary distribution .
Moreover,
where is the first Dirichlet
eigenfunction.
12
One population convergence of stationary
distributions assumptions
Assumption The uniform internal ball condition
13
Two populations convergence to the heat
equation solution
  • population size (same for population I and II)
  • individual particle mass (population I)
  • individual particle mass (population II)
  • empirical density at time
  • individual trajectories follow random walks

Theorem (B, Quastel, 2007) If
then
where is the normalized heat
equation solution with
14
Two populations convergence to the heat
equation solution assumptions
  • Trajectories simple random walks
  • Trajectories reflect at the domain boundary
  • (iii) The two populations have equal sizes
  • (iv) The domain has an analytic boundary

15
Idea of the proof
- n-th Neumann eigenfunction
Main technical challenge bound the clock rate
16
Spectral representation and L1
Lemma. Suppose that D is a domain with
smooth boundary, is the n-th
eigenfunction for the Laplacian with Neumann
boundary conditions and is a signed
measure with a finite total variation.
17
Diffusion in eigenfunction space
Open problem What is the speed of diffusion?
18
Invariance principle for reflected random walks
  • Theorem. Reflected random walk converges
  • to reflected Brownian motion.
  • -domains, Stroock and Varadhan (1971)
  • Uniform domains, B and Chen (2007)

Example Von Koch snowflake is a uniform domain.
Counterexample (B and Chen, 2007) Reflected
random walk does not converge to reflected
Brownian motion in a planar fractal domain.
19
Myopic conditioning
- open, connected, bounded set
- Markov process
- Brownian motion conditioned by
Theorem (B and Chen, 2007). When ,
converge to reflected Brownian
motion in D.
20
  • reflected Brownian motion in

- hitting time of
Problem
21
Definition We will call a bounded set a
trap domain if
22
(No Transcript)
23
Hyperbolic blocks
24
(No Transcript)
25
Theorem (B, Chen and Marshall, 2006) A simply
connected planar domain is a trap domain if
and only if
26
Horn domain
Corollary is a trap domain iff
Example
Trap domain
Write a Comment
User Comments (0)
About PowerShow.com