Analysis
Seminar
|
August 24, 2011
Organizational Meeting
August 31, 2011
Kit Chan, Bowling Green State University
Title: Hypercyclic vectors for the unitary orbit of a hypercyclic
operator
October 5, 2011
Swarup Ghosh, Bowling Green State University
Title: Peak Points and Gleason Parts in R(X) (Part I)
Abstract: Peak points and Gleason parts are two important notions
in the function theory. In this talk, we will first
define peak points and Gleason parts. Then we will
discuss some relations between these two notions. Here
R(X) denotes the uniform closure of the collection of
all rational functions with no poles on C, a compact
subset of the complex plane.
Swarup Ghosh, Bowling Green State University
Title: Peak Points and Gleason Parts in R(X) (Part II)
Abstract: Peak points and Gleason parts are two important notions
in the function theory. Since we have seen the
definition and properties of peak points already, in
this talk, we will first define Gleason parts. Then we
will discuss some relations between these two notions.
Here R(X) denotes the uniform closure of the collection
of all rational functions with no poles on X, a compact
subset of the complex plane.
October 19, 2011
Swarup Ghosh, Bowling Green State University
Title: Peak Points and Gleason Parts in R(X) (Part III)
October 26, 2011
Leonardo Pinheiro, Bowling Green State University
Title: Every Chaotic Operator Satisfies the Hypercyclicity
Criterion
November 2, 2011
Gokul Kadel, Bowling Green State University
Title: Topological Dynamics - Part I
November 9, 2011
Gokul Kadel, Bowling Green State University
Title: Topological Dynamics - Part II
November 16, 2011
Alex Izzo, Bowling Green State University
Title: Function algebras invariant under group actions
Abstract: Motivated by his work on a conjecture of William
Arveson in operator theory, Ronald Douglas raised the
following question, where S denotes the unit sphere in
complex n-space. If A is a function algebra on S that
contains the ball algebra A(S) and whose maximal ideal
space is S, and if A is invariant under the action of
the n-torus on S, does it follow that A = C(S)? We
will discuss the solution to Douglas' question and
present related results that were motivated by the
question.