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19 Noncommutative Geometry
Noncommutative Geometry Speaker: Jason Haradyn (Western) "NCG Learning Seminar: Isospectral and Nonisometric Plane Domains (3)" Time: 14:30 Room: MC 107 As Sunada originally thought of his famous theorem using zeta functions and trace formulae, we will outline how he proved that the almost conjugacy of subgroups implies isospectrality of the manifolds. We will then continue with some important theory and examples of Riemannian orbifolds and construct Buser's example from 1987 of two isospectral, nonisometric flat (not planar) two-dimensional manifolds with boundary, embedded in $\mathbb{R}^{3}$. Finally, we will construct the important planar domain examples by Gordon, Webb and Wolbert in 1992. In addition, we will provide explicit pictures of these domains and subsequent isometric plane domains as constructed by Buser and Conway in 1994. Geometry and Topology
Geometry and Topology Speaker: Timo Schurg (University of Bonn) "Derived Algebraic Cobordism" Time: 15:30 Room: MC 108 I will introduce an extension of Levine and Morel's algebraic
cobordism to (quasi-projective) derived schemes. This extension will have
the additional utility of naturally encompassing virtual fundamental classes
and virtual Gysin homomorphisms. Time permitting, I will discuss the
isomorphism with a different (obvious) extension of algebraic cobordism to
derived schemes that shows any quasi-smooth projective variety is cobordant
to a smooth projective variety. |
20 Analysis Seminar
Analysis Seminar Speaker: Wayne Grey (Western) "Mixed-norm L^P spaces" Time: 15:30 Room: MC 108 Mixed-norm L^P spaces were described by Benedek and Panzone in 1961, but are connected to Littlewood's earlier 4/3 inequality and recent work on the Bohnenblust-Hille inequality. Among these properties are mixed-norm versions of Holder's inequality and Minkowski's integral inequality, which can work together to simplify certain proofs. Minkowski's integral inequality already has a mixed-norm character, and its general mixed-norm extension (described by Fournier in 1987) allows embeddings among various mixed norm spaces on a product measure space. Much of the talk should be clear with a basic background in integration and conventional L^p spaces |
21 Noncommutative Geometry
Noncommutative Geometry Speaker: Asghar Ghorbanppour (Western) "NCG Learning Seminar: Dirac and Generalized Dirac Operators" Time: 14:30 Room: MC 107 For any manifold $M$ with a spin structure $P_{spin}(X)$, we can define a canonical
first order operator, known as the Dirac operator, acting on a spinor bundle. The spinor bundle
is a bundle associated to the spin structure and the representation of spin group, coming from
an irreducible representation of the Clifford algebra. The existence of an irreducible real Clifford
module is equivalent to the existence of a spin structure on the manifold; however, we can
always construct a Dirac bundle, which is (not necessarily irreducible) a $Cl(X)$-module with
compatible metric and connection. Similarly, we may define a differential operator known as
the generalized Dirac operator. In this talk, after some general discussion about Clifford bundles
and Dirac bundles, we will focus on two important examples of the generalized Dirac operator:
the de Rham complex and, in the $4k$-dimensional case, the signature complex. |
22 Colloquium
Colloquium Speaker: Eric Schippers (University of Manitoba) "A correspondence between conformal field theory and Teichmuller theory " Time: 15:30 Room: MC 108 Teichmuller space is a moduli space of Riemann surfaces, where
two Riemann surfaces are equivalent if they are biholomorphic
and are homotopically related in a certain sense. It can be
thought of as the space of local deformations of Riemann surfaces.
Conformal field theories are quantum mechanical or statistical field
theories which are invariant under infinitesimal rotations and
rescalings, and thus in two dimensions they are closely tied to
complex analysis. A mathematical model of conformal field theory
was sketched by Segal and Kontsevich. Attempts to realize this
model rigorously has spawned a great deal of deep mathematics. A certain moduli space in conformal field theory turns out to be
the quotient of Teichmuller space by a discrete group action. This
relation between the two moduli spaces leads to the solution of
analytic problems in the rigorous formulation of conformal field
theory, and new results in Teichmuller theory. In this talk, I
will give a non-technical introduction to the ideas of Teichmuller
theory, and sketch the correspondence between the moduli spaces.
Joint work with David Radnell. |
23 Algebra Seminar
Algebra Seminar Speaker: Nguyen Duy Tan (Western) "Images of additive polynomials" Time: 14:30 Room: MC 108 We study the image of an additive polynomial $f$ over a field $k$ of characteristic
$p > 0$. We define the additive rank of $f$ over $k$ to be the smallest positive integer $r$ such that
there exists an additive polynomial $g$ in $r$ variables with coefficients in $k$ which generates
the same image as $f$ does. We show that over perfect fields the additive ranks of (non-zero) additive
polynomials are always 1. We also show that for every positive integer $r$, there is some
additive polynomial over a certain field with additive rank $r$. Noncommutative Geometry
Noncommutative Geometry Speaker: Mingcong Zeng (Western) "NCG Learning Seminar: A proof of Bott periodicity theorem (1)" Time: 14:30 Room: MC 107 In this talk first I will give some examples of vector bundles on $S^2$ which appears to be very important in complex topological K-theory and show how to imagine them. Then I will define clutching map of vector bundles on $S^n$ which will be used to prove the Bott periodicity. Then
we are prepared to give a definition of K-group and ring structure on it. At last is the statement of Bott periodicity which I will prove in the next week. |
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