10:10
Stochastic Particle Approximation for Measure Valued Solutions of the 2D Keller-Segal System
Abstract
tba
16:00
Unknotting operations on knots and the mapping class group
(HoRSe seminar) Symmetric and reduced obstruction theories
Abstract
I will describe some more of the deformation theory necessary for the first talk. This leads to a number of natural questions and counterexamples. This talk requires a strong stomach, or a fanatical devotion to symmetric obstruction theories.
Tree packing conjectures; Graceful tree labelling conjecture
Abstract
A family of graphs $H_1,...,H_k$ packs into a graph $G$ if there exist pairwise edge-disjoint copies of $H_1,...,H_k$ in $G$. Gyarfas and Lehel conjectured that any family $T_1, ..., T_n$ of trees of respective orders $1, ..., n$ packs into $K_n$. A similar conjecture of Ringel asserts that $2n$ copies of any trees $T$ on $n+1$ vertices pack into $K_{2n+1}$. In a joint work with Boettcher, Piguet, Taraz we proved a theorem about packing trees. The theorem implies asymptotic versions of the above conjectures for families of trees of bounded maximum degree. Tree-indexed random walks controlled by the nibbling method are used in the proof.
In a joint work with Adamaszek, Adamaszek, Allen and Grosu, we used the nibbling method to prove the approximate version of the related Graceful Tree Labelling conjecture for trees of bounded degree.
In the talk we shall give proofs of both results. We shall discuss possible extensions thereof to trees of unbounded degree.
On the existence of modified equations for stochastic differential equations
Abstract
In this talk we describe a general framework for deriving
modified equations for stochastic differential equations with respect to
weak convergence. We will start by quickly recapping of how to derive
modified equations in the case of ODEs and describe how these ideas can
be generalized in the case of SDEs. Results will be presented for first
order methods such as the Euler-Maruyama and the Milstein method. In the
case of linear SDEs, using the Gaussianity of the underlying solutions,
we will derive a SDE that the numerical method solves exactly in the
weak sense. Applications of modified equations in the numerical study
of Langevin equations and in the calculation of effective diffusivities
will also be discussed.
(HoRSe seminar) GW/stable pairs on K3 surfaces
Abstract
(This is joint work with Davesh Maulik and Rahul Pandharipande. Only they understand the actual formulae. People who like modular forms are not encouraged to come to this talk.)
Submarine Hunting and Other Applications of the Mathematics of Tracking
Abstract
12:00
Gravity Quantized
Abstract
Canonical quantization of gravitational field will beconsidered. Examples for which the procedure can be completed (without reducingthe degrees of freedom) will be presented and discussed. The frameworks appliedwill be: Loop Quantum Gravity, relational construction of the Dirac observablesand deparametrization.
Properties of the $C^1$-smooth functions whose gradient range has topological dimension 1
Abstract
In the talk we discuss some results of [1]. We apply our previous methods [2] to geometry and to the mappings with bounded distortion.
\textbf{Theorem 1}. Let $v:\Omega\to\mathbb{R}$ be a $C^1$-smooth function on a domain (open connected set) $\Omega\subset\mathbb{R}^2$. Suppose
$$ (1)\qquad \operatorname{Int} \nabla v(\Omega)=\emptyset. $$
Then $\operatorname{meas}\nabla v(\Omega)=0$.
Here $\operatorname{Int}E$ is the interior of ${E}$, $\operatorname{meas} E$ is the Lebesgue measure of ${E}$. Theorem 1 is a straight consequence of the following two results.
\textbf{ Theorem 2 [2]}. Let $v:\Omega\to\mathbb{R}$ be a $C^1$-smooth function on a domain $\Omega\subset\mathbb{R}^2$. Suppose (1) is fulfilled. Then the graph of $v$ is a normal developing surface.
Recall that a $C^1$-smooth manifold $S\subset\mathbb{R}^3$ is called a normal developing surface [3] if for any $x_0\in S$ there exists a straight segment $I\subset S$ (the point $x_0$ is an interior point of $I$) such that the tangent plane to $S$ is stationary along $I$.
\textbf{Theorem 3}. The spherical image of any $C^1$-smooth normal developing surface $S\subset\mathbb{R}^3$ has the area (the Lebesgue measure) zero.
Recall that the spherical image of a surface $S$ is the set $\{\mathbf{n}(x)\mid x\in S\}$, where $\mathbf{n}(x)$ is the unit normal vector to $S$ at the point~$x$. From Theorems 1--3 and the classical results of A.V. Pogorelov (see [4, Chapter 9]) we obtain the following corollaries Corollary 4. Let the spherical image of a $C^1$-smooth surface $S\subset\mathbb{R}^3$ have no interior points. Then this surface is a surface of zero extrinsic curvature in the sense of Pogorelov.
\textbf{ Corollary 5}. Any $C^1$-smooth normal developing surface $S\subset\mathbb{R}^3$ is a surface of zero extrinsic curvature in the sense of Pogorelov.
\textbf{Theorem 6}. Let $K\subset\mathbb{R}^{2\times 2}$ be a compact set and the topological dimension of $K$ equals 1. Suppose there exists $\lambda> 0$ such that $\forall A,B\in K, \, \, |A-B|^2\le\lambda\det(A-B).$
Then for any Lipschitz mapping $f:\Omega\to\mathbb R^2$ on a domain $\Omega\subset\mathbb R^2$ such that $\nabla f(x)\in K$ a.e. the identity $\nabla f\equiv\operatorname{const}$ holds.
Many partial cases of Theorem 6 (for instance, when $K=SO(2)$ or $K$ is a segment) are well-known (see, for example, [5]).
The author was supported by the Russian Foundation for Basic Research (project no. 08-01-00531-a).
[1] {Korobkov M.\,V.,} {``Properties of the $C^1$-smooth functions whose gradient range has topological dimension~1,'' Dokl. Math., to appear.}
[2] {Korobkov M.\,V.} {``Properties of the $C^1$-smooth functions with nowhere dense gradient range,'' Siberian Math. J., \textbf{48,} No.~6, 1019--1028 (2007).}
[3] { Shefel${}'$ S.\,Z.,} {``$C^1$-Smooth isometric imbeddings,'' Siberian Math. J., \textbf{15,} No.~6, 972--987 (1974).}
[4] {Pogorelov A.\,V.,} {Extrinsic geometry of convex surfaces, Translations of Mathematical Monographs. Vol. 35. Providence, R.I.: American Mathematical Society (AMS). VI (1973).}
[5] {M\"uller ~S.,} {Variational Models for Microstructure and Phase Transitions. Max-Planck-Institute for Mathematics in the Sciences. Leipzig (1998) (Lecture Notes, No.~2. http://www.mis.mpg.de/jump/publications.html).}
15:45
Stochastic nonlinear Schrodinger equations and modulation of solitary waves
Abstract
In this talk, we will focus on the asymptotic behavior in time of the solution of a model equation for Bose-Einstein condensation, in the case where the trapping potential varies randomly in time.
The model is the so called Gross-Pitaevskii equation, with a quadratic potential with white noise fluctuations in time whose amplitude tends to zero.
The initial condition is a standing wave solution of the unperturbed equation We prove that up to times of the order of the inverse squared amplitude the solution decomposes into the sum of a randomly modulatedmodulation parameters.
In addition, we show that the first order of the remainder, as the noise amplitude goes to zero, converges to a Gaussian process, whose expected mode amplitudes concentrate on the third eigenmode generated by the Hermite functions, on a certain time scale, as the frequency of the standing wave of the deterministic equation tends to its minimal value.
14:15
On Rough Path Constructions for Fractional Brownian Motion
Abstract
Abstract: In this talk we will review some recentadvances in order to construct geometric or weakly geometric rough paths abovea multidimensional fractional Brownian motion, with a special emphasis on thecase of a Hurst parameter H<1/4. In this context, the natural piecewiselinear approximation procedure of Coutin and Qian does not converge anymore,and a less physical method has to be adopted. We shall detail some steps ofthis construction for the simplest case of the Levy area.
14:15
Scanning through Heterotic Vacua
Abstract
16:30
Modular Forms, K-theory and Knots
Abstract
Many problems from combinatorics, number theory, quantum field theory and topology lead to power series of a special kind called q-hypergeometric series. Sometimes, like in the famous Rogers-Ramanujan identities, these q-series turn out to be modular functions or modular forms. A beautiful conjecture of W. Nahm, inspired by quantum theory, relates this phenomenon to algebraic K-theory.
In a different direction, quantum invariants of knots and 3-manifolds also sometimes seem to have modular or near-modular properties, leading to new objects called "quantum modular forms".
14:15
Optimal Control Under Stochastic Target Constraints
Abstract
We study a class of Markovian optimal stochastic control problems in which the controlled process $Z^\nu$ is constrained to satisfy an a.s.~constraint $Z^\nu(T)\in G\subset \R^{d+1}$ $\Pas$ at some final time $T>0$. When the set is of the form $G:=\{(x,y)\in \R^d\x \R~:~g(x,y)\ge 0\}$, with $g$ non-decreasing in $y$, we provide a Hamilton-Jacobi-Bellman characterization of the associated value function. It gives rise to a state constraint problem where the constraint can be expressed in terms of an auxiliary value function $w$ which characterizes the set $D:=\{(t,Z^\nu(t))\in [0,T]\x\R^{d+1}~:~Z^\nu(T)\in G\;a.s.$ for some $ \nu\}$. Contrary to standard state constraint problems, the domain $D$ is not given a-priori and we do not need to impose conditions on its boundary. It is naturally incorporated in the auxiliary value function $w$ which is itself a viscosity solution of a non-linear parabolic PDE. Applying ideas recently developed in Bouchard, Elie and Touzi (2008), our general result also allows to consider optimal control problems with moment constraints of the form $\Esp{g(Z^\nu(T))}\ge 0$ or $\Pro{g(Z^\nu(T))\ge 0}\ge p$.
14:00
No workshop in this slot due to OCIAM meeting
Australian Study Group Preview
Abstract
Each problem to be solved at the study group will be discussed.