Tue, 19 Jan 2010

15:45 - 16:45
L3

Big rational surfaces

Damiano Testa
(Oxford)
Abstract

The Cox ring of a variety is an analogue of the homogeneous coordinate ring of projective space. Cox rings are not defined for every variety and even when they are defined, they need not be finitely generated. Varieties for which the Cox ring is finitely generated are called Mori dream spaces and, as the name suggests, they are particularly well-suited for the Minimal Model Program. Such varieties include toric varieties and del Pezzo surfaces.

I will report on joint work with T. Várilly and M. Velasco where we introduce a class of smooth projective surfaces having finitely generated Cox ring. This class of surfaces contains toric surfaces and (log) del Pezzo surfaces.

Thu, 04 Mar 2010
11:00
SR2

Topos Quantum Logic

Andreas Doering
(Oxford)
Abstract

Standard quantum logic, as intitiated by Birkhoff and von Neumann, suffers from severe problems which relate quite directly to interpretational issues in the foundations of quantum theory. In this talk, I will present some aspects of the so-called topos approach to quantum theory, as initiated by Isham and Butterfield, which aims at a mathematical reformulation of quantum theory and provides a new, well-behaved form of quantum logic that is based upon the internal logic of a certain (pre)sheaf topos.

Tue, 10 Nov 2009

14:50 - 15:40
L3

Random graphs with few disjoint cycles

Colin McDiarmid
(Oxford)
Abstract
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Fix a positive integer $k$, and consider the class of all graphs which do not have $k+1$  vertex-disjoint cycles.  A classical result of Erdos and P\'{o}sa says that each such graph $G$ contains a blocker of size at most $f(k)$.  Here a {\em blocker} is a set $B$ of vertices such that $G-B$ has no cycles.

 

We give a minor extension of this result, and deduce that almost all such labelled graphs on vertex set $1,\ldots,n$ have a blocker of size $k$.  This yields an asymptotic counting formula for such graphs; and allows us to deduce further properties of a graph $R_n$ taken uniformly at random from the class: we see for example that the probability that $R_n$ is connected tends to a specified limit as $n \to \infty$.

 

There are corresponding results when we consider unlabelled graphs with few disjoint cycles. We consider also variants of the problem involving for example disjoint long cycles.

 

This is joint work with Valentas Kurauskas and Mihyun Kang.

Tue, 03 Nov 2009

14:30 - 15:30
L3

A general class of self-dual percolation models

Oliver Riordan
(Oxford)
Abstract
One of the main aims in the theory of percolation is to find the `critical probability' above which long range connections emerge from random local connections with a given pattern and certain individual probabilities. The quintessential example is Kesten's result from 1980 that if the edges of the square lattice are selected independently with probability $p$, then long range connections appear if and only if $p>1/2$.  The starting point is a certain self-duality property, observed already in the early 60s; the difficulty is not in this observation, but in proving that self-duality does imply criticality in this setting.

Since Kesten's result, more complicated duality properties have been used to determine a variety of other critical probabilities. Recently, Scullard and Ziff have described a very general class of self-dual percolation models; we show that for the entire class (in fact, a larger class), self-duality does imply criticality.

Mon, 16 Nov 2009

12:00 - 13:00
L3

M2-branes at hypersurface singularities and their deformations

James Sparks
(Oxford)
Abstract
I will introduce a family of supersymmetric Chern-Simons-matter theories in d=2+1 dimensions, labelled by a positive integer n, and argue that these describe the low-energy worldvolume theory of M2-branes at a corresponding family of four-fold hypersurface singularities. There are dual descriptions in Type IIA involving a family of three-fold hypersurface singularities, and also a Type IIB dual of Hanany-Witten type involving D3-branes suspended between 5-branes. The n=1 theory has manifest N=6 superconformal symmetry and is the Aharony-Bergman-Jafferis-Maldacena theory on an M2-brane in flat spacetime. The n>1 theories are not conformal: however, the n>2 theories are all argued to flow to the same superconformal IR fixed point, while the n=2 theory flows to a theory that is AdS/CFT dual to a certain homogeneous Sasaki-Einstein 7-manifold. This is the base of the four-fold "conifold" singularity, and the smooth deformation of this singularity is interpreted as a particular mass deformation in the field theory. The IR theory of this deformation is conjecturally confining.
Fri, 12 Feb 2010

11:30 - 13:00
OCCAM Common Room (RI2.28)

OCCAM group meeting

Various
(Oxford)
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