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Fast
explicit methods for stiff ODEs
September 13
Alexei
Medovikov,
Institute of Numerical Mathematics, Russian Academy of Sciences, Moscow,
Russia
Abstract
Most
of known explicit Runge-Kutta methods has small stability domains -- their
time steps are bounded by a very restrictive CFL condition, and thus standard
explicit methods become useless for stiff ODEs. We propose explicit embedded
integration schemes with large stability domains. The construction of
these methods is achieved in two steps: first, we compute stability polynomials
of a given degree with optimal stability domains, i.e., possessing a Chebyshev
alternation; second, we realize a corresponding explicit Runge-Kutta method
with the help of the theory of Runge-Kutta composition methods.
Reed Solomon Codes: An Application of Abstract and Linear Algebra
January 9
Ivelisse Rubio,
University of Puerto Rico at Humacao
Abstract
Error control codes are used to protect digital information from errors
that can occur during transmission or storage. Reed-Solomon codes are a class of codes that have been widely used in applications such as
satellite transmission and compact disk storage. Their structure as well as encoding and decoding algorithms derived from them can be understood
with an elementary knowledge of linear and abstract algebra.
In this talk I will introduce codes in general and present Reed-Solomon codes from a polynomial ideal point of view.
We will see how concepts and methods from linear and abstract algebra can be used to describe the structure of these
codes and to give encoding and decoding methods. I will also introduce special generating sets for ideals of polynomials
in several variables called "Groebner bases" and I will discuss how they can be used to generalize some of the methods
used in Reed-Solomon codes to encode and decode multidimensional Reed-Solomon codes. Some of these generalizations are
still open problems.
EM travelling Waves and Surface Waves in Photonic Crystal Slabs
January 23
Stefanos Venakides,
Duke University
Abstract
We analyze EM wave propagation and scattering
in photonic crystal slabs, i.e. dielectric structures that are periodic in y and finite in x. They are made with a
material of constant dielectric coefficient embedded in a matrix of another dielectric coeffcient. We study scattering
for polarized incident exponential fields of form exp(iKx+i(m+k)y) where m is an integer, k is the Bloch wavenumber
(real in our analysis), and K is generally complex so that the free dispersion relation K2+(m+k)2=w2 holds, w being
the complex frequency. Developing a boundary integral/boundary element method for periodic structures, we probe
the scattering dispersion relation w=W(k), that holds exactly when the system of linear integral equations that
desribes the scattering acquires a nontrivial nullspace. When the frequency w is real, the null functions correspond
to self-sustained fields that exist in the absence of any incident field and are travelling wave states. We refer
to them as surface waves when most of the field is concentrated at the end of the crystal.
We focus on resonant cases where w has a small negative imaginary part. Although mathematiclly they
correspond to unphysical fields that grow exponentially as x tends to infinity, they cause anomalous
behavior of the scattering states at nearby frequencies at which narrow regions of large resonant fields,
and near-perfect transmission or reflection occur. Both the resonant phenomena and the transmission/
reflection anomalies are absent from scattering states at nearby frequency values when the imaginary
part of the resonant frequency is zero.
Communicating
Mathematics to the Masses (without mangling it)
January 30
Sara Robinson,
Science Writer
Abstract
As a mathematician-turned-mathematics writer, I will draw upon my experience with the New York Times to discuss the perils of effectively and accurately communicating mathematics to the general public and what mathemeticians can do to help.
See samples of New York Times articles written by Sara Robinson
An extension of Hurwitz's zeta function to polyhedral cones in Rn
February 6
Sinai Robins,
Temple University
Abstract
We define an extension of Hurwitz's zeta
function, where the summation index extends to a polyhedral cone in Rn. We find that it has a functional relation,
analogous to the one that Hurwitz found in 1 dimension. The tools are analytic, involving variations of Lipschitz
and Poisson summation in higher dimensions.
Cappell-Shaneson's
4-dimensional s-cobordism
February13
Selman Akbulut,
Michigan State University
Abstract
`Stein-cork
decomposition' and `Lefschetz fibrations' are our main techniques to
study smooth structures of 4-manifolds, but in practice every example
requires its own bag of tricks. We will demonstrate this on Cappell-Shaneson's
celebrated example: In 1987 they had proposed a possible counterexample
to 4-dimensional Poincare Conjecture by constructing a possible nonstandard
s-cobordism from S3 to itself. We show that this
is no counterexample, i.e. the cobordism is the standard product. By
construction, this standard cobordism is the 8-fold covering space of
a strange s-cobordism H from the quaternionic 3-manifold Q to itself.
Potentially H could still be a nonstandard fake s-cobordism. We reduce
the trviality of H to a question about the 3-twist spun trefoil knot
in S4, and
also relate this to a question about a Fintushel-Stern knot surgery.
Numerical methods for compressible multimaterial flows
February20
Smadar Karni,
University of Michigan
Abstract
Multimaterial flows are of great interest in a
wide variety of physical problems, ranging from studying the dynamics and stability of interfaces, through mixing processes,
the dynamics of bubbles, to liquid suspensions and bubbly flows. Different types of flows call for different assumptions,
and lead to flow models which raise computational issues of different flavor.
Stratified flows dominated by propagating material fronts are often described by one-velocity one-pressure models.
Unexpectedly, numerical methods for these models have proved difficult, often producing material fronts contaminated
by nonphysical oscillations. In dispersed flows, such as liquid suspensions, tracking individual interfaces is not of
interest for the macroscopic flow description. A common practice is to average the equations, yielding models that are
inherently nonconservative due to momentum and energy exchange terms between the phases. They require closure relations
which are not available from first physical principles, and even when motivated by physical considerations yield
controversial results. Most notoriously, assuming a single (equilibrium) pressure for all species, leads to loss of
time-hyperbolicity of the governing equations, often referred to as the ill-posedness of the multiphase flow equations.
The talk will discuss the numerical issues raised by multimaterial flow computations, will present strategies
in the design of suitable numerical algorithms and a host of numerical results.
An analogue
of Abel's theorem
February 27
Herb Clemens,
Ohio State University
Abstract
Abel's classical theorem giving
the condition that formal sums of points on a Riemann surfaces may be the zero (polar) set of a rational
function `almost' has an analogue for sums of curves on a three-dimensional Kaehler manifold. The role of
complex line bundles in the modern interpretation of Abel's theorem is played by `quaternionic line bundles.'
The octic equation and beyond
March 13
Scott Crass,
CSULB
Abstract
The requirement for solving a polynomial is a
means of breaking its symmetry, which in the case of the octic, is that of the symmetric group S8. Its eight-dimensional
linear permutation representation restricts to a six-dimensional projective action. A mapping of complex projective
6-space with this S8 symmetry can provide the requisite symmetry-breaking tool.
The talk will describe some of the S8 geometry in CP6 as well as a S8-symmetric rational map with special geometric
and dynamical properties. An explicit algorithm that uses this map to solve a general octic will run in real time.
A concluding discussion will treat the generality of this approach.
On the
distance function to the boundary and the singular set of solutions of
some Hamilton Jacobi equations
March 20
Louis Nirenberg,
Courant Institute
Clifford Lectures March 27
Constrained Dynamics, Conservation Laws, and Control
April 3
Dmitry Zenkov,
North Carolina State University
Abstract
This talk will overview some modern trends in dynamics and control of constrained systems.
The behavior of such systems is often counterintuitive. For example, in the absence of external
dissipation such systems conserve energy but nonetheless can exhibit asymptotically stable
relative equilibria. Another interesting behavior which does not occur in unconstrained systems
is that symmetries do not always lead to momentum conservation laws as in the classical Noether
theorem. Instead, the momentum satisfies a dynamic momentum equation. Conditions for conservation
of some of the components of the momentum will be discussed. Usability of both the presence and lack
of conservation laws in control will then be covered.
Links to other archived years...
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April 15, 2005
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