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1 Noncommutative Geometry
Noncommutative Geometry Speaker: Travis Ens (Western) "NCG Learning Seminar: Path Integrals in Quantum Mechanics (4)" Time: 14:30 Room: MC 107 By transforming to momentum space, the integrals used to compute
the Feynman weight of a graph can be simplified. After carrying out this process,
I will compute the partition function of two simple systems, quantum mechanics on
a circle and circle-valued quantum mechanics. Finally I will discuss how these methods
easily generalize to quantum field theory in the case of a free scalar bosonic field. |
2 Analysis Seminar
Analysis Seminar Speaker: Dayal Dharmasena (Syracuse University) "Holomorphic Fundamental Semigroup of Riemann Domains" Time: 15:30 Room: MC 108 Let (W,Π) be a Riemann domain over a complex manifold M and w0 be a point in W. Let D be the unit disk in C and T=∂D. Consider the space S1,w0(¯D,W,M) of continuous mappings f of T into W such that f(1)=w0 and Π∘f extends to a holomorphic on D mapping ˆf. Mappings f0,f1∈S1,w0(¯D,W,M) are called {\it holomorphically homotopic or h-homotopic} if there is a continuous mapping ft of [0,1] into S1,w0(¯D,W,M). Clearly, the h-homotopy is an equivalence relation and the equivalence class of f∈S1,w0(¯D,W,M) will be denoted by [f] and the set of all equivalence classes by η1(W,M,w0).
\par There is a natural mapping ι1:η1(W,M,w0)→π1(W,w0) generated by assigning to f∈S1,w0(¯D,W,M) its restriction to T. We introduce on η1(W,M,w0) a binary operation ⋆ which induces on η1(W,M,w0) a structure of a semigroup with unity and show that η1(W,M,w0) is an algebraic biholomorphic invariant of Riemann domains. Moreover, ι1([f1]⋆[f2])=ι1([f1])⋅ι1([f2]), where ⋅ is the standard operation on π1(W,w0). Then we establish standard properties of η1(W,M,w0) and provide some examples. When W is a finitely connected domain in M=C and Π is the identity, we show that ι1 is an isomorphism of η1(W,M,w0) onto the minimal subsemigroup of π1(W,w0) containing holomorphic generators and invariant with respect to the inner automorphisms. In particular, we show for a general domain W⊂C that [f1]=[f2] if and only if ι1([f1])=ι1([f2]). This is a joint work with Evgeny Poletsky.
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3 Noncommutative Geometry
Noncommutative Geometry Speaker: Masoud Khalkhali (Western) "Localization in equivariant cohomology and index formula" Time: 14:30 Room: MC 107 The path integral formula for the index of the Dirac operator can be interpreted as a
localization formula for U(1)-equivariant cohomology of the free loop space of the manifold.
In this lecture I shall first recall the Cartan model of equivariant differential forms of a finite
dimensional manifold and the localization formula of Berline-Vergne. We shall then see that the
loop space analogue of this result will give the A hat genus. This can be regarded as the bosonic
component of the index formula. The corresponding localization formula in the supersymmetric
case gives the full index formula. |
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5 Noncommutative Geometry
Noncommutative Geometry Speaker: Asghar Ghorbanpour (Western) "NCG Learning Seminar: Applications of the Atiyah-Singer Index theorem 4: the Hirzebruch-Riemann-Roch Theorem" Time: 10:30 Room: MC 107 Following the previous talks on the Atiyah-Singer index theorem by Masoud, we will prove
another important special case, namely the Hirzebruch-Riemann-Roch theorem. This theorem gives the
holomorphic Euler characteristic of a holomorphic vector bundle over a compact Kähler manifold in terms
of the Todd class of the manifold and the Chern character of the vector bundle. It will be shown how in the
case of a holomorphic line bundle over a Riemann surface this reduces to the classical Riemann-Roch theorem. Algebra Seminar
Algebra Seminar Speaker: David Riley (Western) "On the behaviour of the Frobenius map in a noncommutative world" Time: 14:30 Room: MC 108 |
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