Gaussian fluctuations for Plancherel partitions

Speaker: 

Professor Leonid Bogachev

Institution: 

University of Leeds, UK

Time: 

Tuesday, October 12, 2010 - 11:00am

Location: 

RH 306

The limit shape of Young diagrams under the Plancherel
measure was found by Vershik \& Kerov (1977) and Logan \& Shepp
(1977). We obtain a central limit theorem for fluctuations of Young
diagrams in the bulk of the partition '`spectrum''. More
specifically, under a suitable (logarithmic) normalization, the
corresponding random process converges (in the FDD sense) to a
Gaussian process with independent values. We also discuss a link
with an earlier result by Kerov (1993) on the convergence to a
generalized Gaussian process. The proof is based on poissonization
of the Plancherel measure and an application of a general central
limit theorem for determinantal point processes. (Joint work with
Zhonggen Su.)

scaling exponents for a one-dimensional directed polymer

Speaker: 

Professor Timo Seppalainen

Institution: 

University of Wisconsin

Time: 

Wednesday, June 2, 2010 - 2:00pm

Location: 

MSTB 114

We study a 1+1-dimensional directed polymer in a random
environment on the integer lattice with log-gamma distributed
weights and both endpoints of the polymer path fixed.
We show that under appropriate boundary conditions
the fluctuation exponents for the free energy and
the polymer path take the values conjectured in the
theoretical physics literature. Without the boundary
we get the conjectured upped bounds on the exponents.

A propagation-of-chaos type result in stochastic averaging

Speaker: 

Professor Richard Sowers

Institution: 

University of Illinois

Time: 

Tuesday, May 25, 2010 - 11:00am

Location: 

RH 306

Stochastic averaging goes back to Khasminskii in the 1960's. The
standard result is that, given a separation of scales, one can find effective dynamics
for slow components. We investigate the motion of two particles in such a system, in
particular in a randomly-perturbed twist map. The nub of the issue
is how two points escape from a 1-1 resonance zone. Results of Pinsky
and Wihstutz indicate that there is a third scale at work, which we can use to study
the escape from resonance.

The Ghirlanda-Guerra identities and ultrametricity in the Sherrington-Kirkpatrick model.

Speaker: 

Professor Dmitry Panchenko

Institution: 

Texas A&M

Time: 

Monday, May 10, 2010 - 11:00am

Location: 

RH 306

The Parisi theory of the Sherrington-Kirkpatrick model completely describes the geometry of the Gibbs sample in a sense that it predicts the limiting joint distribution of all scalar products, or overlaps, between i.i.d. replicas. One of the main predictions is that asymptotically the Gibbs measure concentrates on an ultrametric subset of all spin configurations. Another part of the theory are the Ghirlanda-Guerra identities which in various formulations have been proved rigorously. It is well known that together these two properties completely determine the joint distribution of the overlaps and for this reason they were always considered complementary. We show that in the case when overlaps take finitely many values the Ghirlanda-Guerra identities actually imply ultrametricity.

On the existence and position of the farthest peaks of a family of stochastic heat and wave equations.

Speaker: 

Professor Davar Khoshnevisan

Institution: 

University of Utah

Time: 

Tuesday, April 20, 2010 - 11:00am

Location: 

RH 306

We study the stochastic heat equation ∂tu = u+σ(u)w in (1+1) dimensions, where w is space-time white noise, σ:R→R is Lipschitz continuous, and is the generator of a Lvy process. We assume that the underlying Lvy process has finite exponential moments in a neighborhood of the origin and u0 has exponential decay at ∞. Then we prove that under natural conditions on σ: (i) The νth absolute moment of the solution to our stochastic heat equation grows exponentially with time; and (ii) The distances to the origin of the farthest high peaks of those moments grow exactly linearly with time. Very little else seems to be known about the location of the high peaks of the solution to the stochastic heat equation. Finally, we show that these results extend to the stochastic wave equation driven by Laplacian.
This is joint work with Daniel Conus (University of Utah)

Stein's Method for the Lightbulb Process (Larry Goldstein and Haimeng Zhang)

Speaker: 

Professor Larry goldstein

Institution: 

USC

Time: 

Tuesday, March 2, 2010 - 11:00am

Location: 

RH 306

In the so called light bulb process of Rao, Rao and Zhang (2007), on days r =
1, . . . , n, out of n light bulbs, all initially off, exactly r bulbs, selected uniformly and
independent of the past, have their status changed from off to on or vice versa. With
X the number of bulbs on at the terminal time n, an even integer and = n/2, σ2 =
varX, we have
sup
∈R 􏰐
􏰐
P ( X −
σ ≤ z ) − P (Z ≤ z )
􏰐􏰐 ≤
n
2σ2 ∆0 + 1.64
n
σ3 +
2
σ
where Z is a
N (0, 1) random variable and
∆0
≤
1
2√n +
1
2n + e−
n/2
, for n
≥ 4,
yielding a bound of order O(n−1/2 ) as n
→ ∞.
The results are shown using a version of Steins method for bounded, monotone
size bias couplings. The argument for even n depends on the construction of a variable
X s on the same space as X which has the X size bias distribution, that is, which
satisfies
E[X g(X )] = E[g(X s )], for all bounded continuous g
and for which there exists a B
≥ 0, in this case, B = 2, such that X ≤ X
s
≤ X + B
almost surely. The argument for odd n is similar to that for n even, but one first
couples X closely to V , a symmetrized version of X, for which a size bias coupling of
V to V s can proceed as in the even case.

What equation does a diffusing particle obey?

Speaker: 

Professor Janek Wehr

Institution: 

University of Arizona

Time: 

Friday, February 12, 2010 - 11:00am

Location: 

RH 306

Motion of a Brownian particle in a force field is described in the Smoluchowski-Kramers approximation by a stochastic differential
equation---Langevin equation.
If the diffusion coefficient depends on the particle's position, this equation is ambiguous due to several possible interpretations
of the stochastic differential. Two most often used interpretations are those of Ito and Stratonovitch, so the problem
is sometimes called the Ito-Stratonovitch dilemma. I will discuss the results of a recent experiment, which determine what
is the correct interpretation of the Langevin equation and show how they are consistent mathematically with the
Smoluchowski-Kramers approximation. Possible implications for studying a class of stochastic differential equations will
be mentioned.

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