Seminars and Colloquia by Series

Monday, September 28, 2009 - 14:00 , Location: Skiles 269 , Vera Vertesi , MSRI , Organizer: John Etnyre
Legendrian knots are knots that can be described only by their projections(without having to separately keep track of the over-under crossinginformation): The third coordinate is given as the slope of theprojections. Every knot can be put in Legendrian position in many ways. Inthis talk we present an ongoing project (with Etnyre and Ng) of thecomplete classification of Legendrian representations of twist knots.
Monday, September 21, 2009 - 14:00 , Location: Skiles 269 , Doug LaFountain , SUNY - Buffalo , Organizer: John Etnyre
The uniform thickness property (UTP) is a property of knots embeddedin the 3-sphere with the standard contact structure. The UTP was introduced byEtnyre and Honda, and has been useful in studying the Legendrian and transversalclassification of cabled knot types.  We show that every iterated torus knotwhich contains at least one negative iteration in its cabling sequence satisfiesthe UTP.  We also conjecture a complete UTP classification for iterated torusknots, and fibered knots in general.
Monday, September 14, 2009 - 15:00 , Location: Skiles 269 , Christian Zickert , UC Berkeley , zickert@math.berkeley.edu , Organizer: Stavros Garoufalidis
A closed hyperbolic 3-manifold $M$ determines a fundamental classin the algebraic K-group $K_3^{ind}(C)$. There is a regulator map$K_3^{ind}(C)\to C/4\Pi^2Z$, which evaluated on the fundamental classrecovers the volume and Chern-Simons invariant of $M$. The definition of theK-groups are very abstract, and one is interested in more concrete models.The extended Bloch is such a model. It is isomorphic to $K_3^{ind}(C)$ andhas several interesting properties: Elements are easy to produce; thefundamental class of a hyperbolic manifold can be constructed explicitly;the regulator is given explicitly in terms of a polylogarithm.
Monday, September 14, 2009 - 14:00 , Location: Skiles 269 , Dishant M. Pancholi , International Centre for Theoretical Physics, Trieste, Italy , Organizer: John Etnyre
 After reviewing a few techniques from the theory of confoliation in dimension three we will discuss some generalizations and certain obstructions in extending these techniques to higher dimensions. We also will try to discuss a few questions regarding higher dimensional confoliations. 
Monday, September 7, 2009 - 14:00 , Location: - , - , - , Organizer: John Etnyre
Monday, August 31, 2009 - 14:01 , Location: Skiles 269 , Rinat Kashaev , Section de Mathématiques Université de Genève , Rinat.Kashaev@unige.ch , Organizer: Stavros Garoufalidis
Not yet!
Monday, April 20, 2009 - 13:00 , Location: Skiles 269 , Scott Baldridge , LSU , Organizer: John Etnyre
In this talk we will introduce the notion of a cube diagram---a surprisingly subtle, extremely powerful new way to represent a knot or link. One of the motivations for creating cube diagrams was to develop a 3-dimensional "Reidemeister's theorem''. Recall that many knot invariants can be easily be proven by showing that they are invariant under the three Reidemeister moves. On the other hand, simple, easy-to-check 3-dimensional moves (like triangle moves) are generally ineffective for defining and proving knot invariants: such moves are simply too flexible and/or uncontrollable to check whether a quantity is a knot invariant or not. Cube diagrams are our attempt to "split the difference" between the flexibility of ambient isotopy of R^3 and specific, controllable moves in a knot projection. The main goal in defining cube diagrams was to develop a data structure that describes an embedding of a knot in R^3 such that (1) every link is represented by a cube diagram, (2) the data structure is rigid enough to easily define invariants, yet (3) a limited number of 5 moves are all that are necessary to transform one cube diagram of a link into any other cube diagram of the same link. As an example of the usefulness of cube diagrams we present a homology theory constructed from cube diagrams and show that it is equivalent to knot Floer homology, one of the most powerful known knot invariants.
Monday, April 13, 2009 - 14:00 , Location: Skiles 269 , Roman Golovko , USC , Organizer: John Etnyre
We will define the sutured version of embedded contact homology for sutured contact 3-manifolds. After that, we will show that the sutured version of embedded contact homology of S^1\times D^2, equipped with 2n sutures of integral or infinite slope on the boundary, coincides with the sutured Floer homology.
Monday, April 13, 2009 - 13:00 , Location: Skiles 269 , Uli Walther , Purdue University , Organizer: Stavros Garoufalidis
Starting with some classical hypergeometric functions, we explain how to derive their classical univariate differential equations. A severe change of coordinates transforms this ODE into a system of PDE's that has nice geometric aspects. This type of system, called A-hypergeometric, was introduced by Gelfand, Graev, Kapranov and Zelevinsky in about 1985. We explain some basic questions regarding these systems. These are addressed through homology, combinatorics, and toric geometry.
Monday, April 6, 2009 - 16:00 , Location: Emory, W306 MSC (Math and Science Center) , Noel Brady , University of Oklahoma , Organizer: John Etnyre

Joint meeting at Emory

A k--dimensional Dehn function of a group gives bounds on the volumes of (k+1)-balls which fill k--spheres in a geometric model for the group. For example, the 1-dimensional Dehn function of the group Z^2 is quadratic. This corresponds to the fact that loops in the euclidean plane R^2 (which is a geometric model for Z^2) have quadratic area disk fillings. In this talk we will consider the countable sets IP^{(k)} of numbers a for which x^a is a k-dimensional Dehn function of some group. The situation k \geq 2 is very different from the case k=1.

Pages