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Mathematics and Statistics Departmental ColloquiumRoom 1634, Lederle Graduate Research TowerUniversity of Massachusetts, Amherst |
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Refreshments at 3:45pm.
Talks begin at 4:00pm.
Driving Directions and
Campus Map
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| Maintained by Frank Sottile. |
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12 September | Jonathon Weitsman, University of California at Santa Cruz | |
| 4:00-5:00 | The topology of Hamiltonian Loop Group spaces. | ||
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19 September | Markus Schmies, Technische Universität Berlin | |
| 4:00-5:00 | Java Oorange: a laboratory for experimental programming in science | ||
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26 September | Paola Sebastini, U Mass | |
| 4:00-5:00 | Statistical challenges in the post-genome era | ||
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3 October | Allen Knutson, University of California at Berkeley and Gregory Warrington, University of Massachusetts | |
| 4:00-5:00 | Mathematics of Juggling | ||
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10 October | Amherst College CVC Refreshments at 4:00 PM in 206 Seeley-Mudd | |
| 4:30-5:30 | Frank Morgan, Williams College (208 Seeley-Mudd) | ||
| Double Bubbles Past, Present, and Future. | |||
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17 October | Randy McCarthy, University of Illinois at Urbana-Champaign | |
| 4:00-5:00 | Classical algebra via Calculus | ||
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24 October | William Graham, University of Georgia | |
| 2:30-3:30 | Degeneracy loci: linear algebra, geometry, and combinatorics | ||
| Time Change Due to Talk of John Nash | |||
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31 October | No colloquium | |
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6 November | Alexandar Bobenko, | |
| 4:30-5:30 | Cancelled: Delay in Visa | ||
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7 November | Wendell Fleming, Brown University | |
| 4:00-5:00 | Max-Plus Stochastic Control | ||
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14 November | Augustin Banyaga, Penn State University | |
| 4:00-5:00 | Locally conformal symplectic structures | ||
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21 November | Joel Lebowitz, Rutgers University Earlier than usual! | |
| 3:30-4:30 | The Meaning and Uses of Entropy | ||
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28 November | No Coloquium: Thanksgiving | |
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5 December | Nantel Bergeron, York University, Toronto, Canada | |
| 4:00-5:00 | Quasi-symmetric polynomials and Temperley-Lieb invariants and covariants | ||
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12 December | Constantine Dafermos, Brown University | |
| 4:00-5:00 | A new approach to the Riemann problem for hyperbolic conservation laws | ||
Abstract
Let M be a Hamiltonian G-space; that is,
a symplectic manifold equipped with a Hamiltonian
action of a compact Lie group G. A theorem of Kirwan,
inspired by the ideas of Atiyah and Bott, shows that
the square of the moment map is an equivariantly perfect Morse function
on M. As a consequence, the equivariant cohomology of
M provides a set of generators for the cohomology of
the reduced space M//G (Kirwan's surjectivity theorem).
We study an analog of this theorem in the case of infinite dimensional symplectic manifolds, equipped with a Hamiltonian action of a loop group LG, where G is a compact Lie group. We show that, in an appropriate sense, the square of the moment map is an equivariantly perfect Morse function on such a space. Similarly, there is an analog of Kirwan's surjectivity theorem.
Examples of such spaces are coadjoint orbits of the loop group (where the Morse function is the classical energy functional of Morse and Bott) and spaces arising from Yang-Mills theory in two dimensions.
(joint work with R. Bott and S. Tolman)
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Abstract
Experiments play a key role in science.
This is reflected in the way that most scientific software is developed.
On the one hand there is the scientific question that has to be solved,
on the other the need to verify the suitability and correctness of the methods used.
Together these aspects combine to a workflow we call experimental programming.
The experience of more than ten years research at the TU Berlin has yielded a tool
offering an environment which hopefully matches the requirements resulting from the
workflow described above: Oorange.
This talk will briefly discuss the concepts of Oorange and the technical background,
including reference to Java.
The workflow of experimental programming with Oorange will be demonstrated by examples.
These include one illustration developed completely from scratch,
and real-life examples from current research projects.
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Abstract
On February 12, 2001 leaders of the Human Genome Project announced the
completion of a draft of the human genome. The result of these efforts
is a map of the human genes, and because about 50% of discovered genes
have known functions, the challenge now is to annotate this map, by
discovering the functions of genes, and their interplay with proteins
and the environment to create complex, dynamic living systems. This is
the goal of functional genomics.
The modern approach to functional genomics takes advantage of the new
technology of microarrays to observe the genome of an entire organism in
action by simultaneously measuring the level of expression of thousands
of genes under the same experimental condition. Microarray technology is
used in simple comparative experiments, when the goal is to identify the
genes that are differentially expressed in cells of the same tissue in
two different conditions. More ambitious experiments try to discover
gene functions or gene interactions from temporal or multifactor
experiments. The design and analysis of these experiments require the
development of new modeling and computational techniques, and this talk
will describe some of the recent methodology we developed for the
analysis of microarray data.
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Abstract
Around 1985, several jugglers independently invented the same
mathematical theory of juggling patterns. In addition to aiding in
the categorization, recording and enumeration of patterns, this
description of patterns has facilitated the discovery of worthwhile
new ones. The theory will be presented with ample demonstrations. As
time permits, we will introduce the combinatorial and probabilistic
questions suggested by this viewpoint. No juggling knowledge will be
assumed.
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Abstract
Goodwillie's calculus of functors has a similar goal as
the ordinary calculus of functions: use linear (additive) methods
to study non-linear phenonema. Its context though is in the realm
of modern algebra, and a basic object is the Taylor tower of
a functor. New criteria are developed jointly with
Kristen Baxter for Taylor towers to split into their layers.
Our primary objective is to introduce the audience to this
calculus of functors via a simple construction due to work
with Brenda Johnson and to show via examples what kind of
information the associated Taylor tower produces. We will
also discuss how this splitting unifies several classical
results of homological algebra.
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Abstract
This talk concerns a broad class of algebraic varieties
defined by conditions involving linear algebra -- more precisely, the
linear algebra of vector bundles. For example, let X denote the set
of all n by n complex matrices, and let Xr
denote the set of
matrices whose rank is at most r. Then the set of matrices with
rank n is a dense
open set in X -- a "generic" matrix has rank n.
Each of the Xr
is a set of degenerate matrices, the most degenerate being X0,
which is simply the zero matrix. Algebraic varieties defined by
conditions such as these are called degeneracy loci. They lie at the
intersection of linear algebra, geometry, and combinatorics.
In this talk I will discuss three types of questions about degeneracy
loci. (1) When are sets defined by degeneracy conditions nonempty?
(2) If a degeneracy locus is a finite set of points, how can one
calculate the number of points? More generally, how can one make
cohomology calculations? (3) Some topological questions about
degeneracy loci have been reduced to combinatorics. For example, in
some cases one can use combinatorics to tell if a degeneracy locus is
smooth. Are there ways to make the combinatorial calculations more
efficient?
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Abstract
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Abstract
We discuss symplectic, contact and locally conformal symplectic structures.
We show how they are connected and how they organize themselves inside
the category of Jacobi structures.
An emphasis is put on the role of their automorphism groups
since they encode the corresponding geometries in the spirit of
the Erlanger Programme.
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Abstract
According to the second law of thermodynamics (Clausius 1857) the entropy
S(M) of an isolated macroscopic system passing from an equilibrium state
specified by parameters M1 (energy, volume, etc.) to another equilibrium
state with parameters M2 must satisfy the inequality
S(M2) \geq
S(M1):
the entropy S(M) of an equilibrium system is defined
operationally. A microscopic expression for S(M),
which also provides an understanding of the origin of the second law, was
given by Boltzmann:
S(M) =
{log of the phase space volume corresponding to M}.
These equilibrium expression for S(M) naturally
generalize to systems in local equilibrium with parameters
M(x,t)
varying slowly (on a microscopic scale) in space and time: this includes
fluids in turbulent motion. Note that S(M) is defined for individual
macroscopic systems and does not require probability distributions or
ensembles: the generalization of the microscopic definition to quantum
systems requires some care.
Boltzmann also defined an entropy function Sgas({f}) for a
dilute gas far from local equilibrium, where f(x, v,t) is the
density of gas particles in the six-dimensional m-space, and showed that
this increases monotonically with time. Sgas({f}) =
{log of phase space volume corresponding to f}:
Sgas({feq}) = S(M).
A similar useful definition of entropy for general systems far
from local equilibrium, i.e. for systems in which correlations are
important, is still very much an open problem. I will describe recent work
on large deviations in stationary nonequilibrium states which has some
bearing on this problem.
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Abstract
Quasi-symmetric polynomials were introduced in enumerative
combinatorics by Gessel and Stanley for the enumeration of P-partitions.
Recent developments show that these
polynomials can be view as Temperley-Lieb polynomials invariants.
We will recall the basic facts on quasi-symmetric polynomials and survey
some of the striking recent developments concerning them.
We will also look at the Temperley-Lieb analogue of the diagonally symmetric
polynomials and the diagonally symmetric harmonics.
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Abstract
This lecture will survey the classical approach for solving the
Riemann problem for hyperbolic systems of conservation laws, and
will discuss a new method of solution, based on a variational principle.
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