Thu, 01 Mar 2012

13:00 - 14:00
L3

Applications of non-linear analysis to geometry

Robert Clancy
Abstract

I will claim (and maybe show) that a lot of problems in differential geometry can be reformulated in terms of non-linear elliptic differential operators. After reviewing the theory of linear elliptic operators, I will show what can be said about the non-linear setting.

Tue, 21 Feb 2012

15:45 - 16:45
L3

Quadratic differentials as stability conditions

Tom Bridgeland
(Oxford)
Abstract

I will explain how moduli spaces of quadratic differentials on Riemann surfaces can be interpreted as spaces of stability conditions for certain 3-Calabi-Yau triangulated categories. These categories are defined via quivers with potentials, but can also be interpreted as Fukaya categories. This work (joint with Ivan Smith) was inspired by the papers of  Gaiotto, Moore and Neitzke, but connections with hyperkahler metrics, Fock-Goncharov coordinates etc. will not be covered in this talk.

Tue, 28 Feb 2012

14:30 - 15:30
L3

On packing and covering in hypergraphs

Penny Haxell (Waterloo)
Abstract

We discuss some recent developments on the following long-standing problem known as Ryser's

conjecture. Let $H$ be an $r$-partite $r$-uniform hypergraph. A matching in $H$ is a set of disjoint

edges, and we denote by $\nu(H)$ the maximum size of a matching in $H$. A cover of $H$ is a set of

vertices that intersects every edge of $H$. It is clear that there exists a cover of $H$ of size at

most $r\nu(H)$, but it is conjectured that there is always a cover of size at most $(r-1)\nu(H)$.

Tue, 06 Mar 2012

14:30 - 15:30
L3

Random graphs on spaces of negative curvature

Nikolaos Fountoulakis (Birmingham)
Abstract

Random geometric graphs have been well studied over the last 50 years or so. These are graphs that

are formed between points randomly allocated on a Euclidean space and any two of them are joined if

they are close enough. However, all this theory has been developed when the underlying space is

equipped with the Euclidean metric. But, what if the underlying space is curved?

The aim of this talk is to initiate the study of such random graphs and lead to the development of

their theory. Our focus will be on the case where the underlying space is a hyperbolic space. We

will discuss some typical structural features of these random graphs as well as some applications,

related to their potential as a model for networks that emerge in social life or in biological

sciences.

Tue, 14 Feb 2012

14:30 - 15:30
L3

Line arrangements and geometric representations of graphs

Tobias Mueller, Amsterdam
Abstract

A dot product representation of a graph assigns to each vertex $s$ a vector $v(s)$ in ${\bf R}^k$ in such a way that $v(s)^T v(t)$ is greater than $1$ if and only $st$ is an edge. Similarly, in a distance representation $|v(s)-v(t)|$ is less than $1$ if and only if $st$ is an edge.

I will discuss the solution of some open problems by Spinrad, Breu and Kirkpatrick and others on these and related geometric representations of graphs. The proofs make use of a connection to oriented pseudoline arrangements.

(Joint work with Colin McDiarmid and Ross Kang)

Mon, 07 May 2012

12:00 - 13:00
L3

Integer Partitions, Mirror Symmetry and 3d Gauge Theories

Noppadol Mekareeya
(Max Planck Institut fuer Physik)
Abstract

In this talk, I will focus on an infinite class of 3d N=4 gauge theories

which can be constructed from a certain set of ordered pairs of integer

partitions. These theories can be elegantly realised on brane intervals in

string theory.  I will give an elementary review on such brane constructions

and introduce to the audience a symmetry, known as mirror symmetry, which

exchanges two different phases (namely the Higgs and Coulomb phases) of such

theories.  Using mirror symmetry as a tool, I will discuss a certain

geometrical aspect of the vacuum moduli spaces of such theories in the

Coulomb phase. It turns out that there are certain infinite subclasses of

such spaces which are special and rather simple to study; they are complete intersections. I will mention some details and many interesting features of these spaces.

Mon, 20 Feb 2012

15:45 - 16:45
L3

Free and linear representations of Out(F_n)

Dawid Kielak
(Oxford)
Abstract

For a fixed n we will investigate homomorphisms Out(F_n) to

Out(F_m) (i.e. free representations) and Out(F_n) to

GL_m(K) (i.e. K-linear representations). We will

completely classify both kinds of representations (at least for suitable

fields K) for a range of values $m$.

Tue, 21 Feb 2012

14:30 - 15:30
L3

Lion and Man: Can both win?

Mark Walters
Abstract

Rado introduced the following `lion and man' game in the 1930's: two players (the lion and the man) are in the closed unit disc and they can run at the same speed. The lion would like to catch the man and the man would like to avoid being captured.

This game has a chequered history with several false `winning strategies' before Besicovitch finally gave a genuine winning strategy.

We ask the surprising question: can both players win?

Tue, 21 Feb 2012
12:00
L3

Correlation functions, Wilson loops, and local operators in twistor space

Tim Adamo
(Oxford)
Abstract

Abstract:

Motivated by the correlation functions-Wilson loop correspondence in maximally supersymmetric Yang-Mills theory, we will investigate a conjecture of Alday, Buchbinder, and Tseytlin regarding correlators of null polygonal Wilson loops with local operators in general position.  By translating the problem to twistor space, we can show that such correlators arise by taking null limits of correlation functions in the gauge theory, thereby providing a proof for the conjecture.  Additionally, twistor methods allow us to derive a recursive formula for computing these correlators, akin to the BCFW recursion for scattering amplitudes.

Tue, 28 Feb 2012
12:00
L3

Peeling of the Weyl tensor and gravitational radiation in higher dimensions.

Mahdi Godazgar
(DAMTP, Cambridge)
Abstract

Abstract: In this talk, I will discuss the peeling behaviour of the Weyl tensor near null infinity for asymptotically flat higher dimensional spacetimes. The result is qualitatively different from the peeling property in 4d. Also, I will discuss the rewriting of the Bondi energy flux in terms of "Newman-Penrose" Weyl components.

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