Topological vertex and geometric transitions via BeilinsonDrinfeld topological chiral algebra

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Topological vertex and geometric transitions via BeilinsonDrinfeld topological chiral algebra

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Brief review of topological vertex and its mathematics ... Duistermaat-Heckman-Atiyah-Bott-Witten (Duistermaat-Heckman: Invent. Math. ... –

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Title: Topological vertex and geometric transitions via BeilinsonDrinfeld topological chiral algebra


1
Topological vertex and geometric transitions via
Beilinson-Drinfeld topological chiral algebra
  • Makoto Sakurai
  • Particle Theory Group, Hongo, the University of
    Tokyo

2
Table of contents
  • Brief review of topological vertex and its
    mathematics
  • Vertex operators induced from moduli spaces
    (topological chiral algebra)
  • A-model lattice Heisenberg algebra
  • B-model W-algebra and BRST reduction
  • Relations between two moduli spaces Ziv Ran
    versus Simpson

3
Chapter 1Review of topological vertices
  • The Topological Vertex (hep-th/0305132)
  • Aganagic-Klemm-Mariño-Vafa
  • Open / Closed string duality
  • Through large Nc limit of Chern-Simons gauge
    theory
  • One way to define the open Gromov-Witten
    invariants

4
Geometric moduli theory
  • Localization theorem localization on the moduli
    space
  • Duistermaat-Heckman-Atiyah-Bott-Witten
    (Duistermaat-Heckman Invent. Math. 69 (1982)
    259, Witten hep-th/9204083)
  • Instanton calculus of moduli of Yang-Mills
  • (closed / open) Gromov-Witten invariants are
    defined in terms of algebraic curves

5
Vertex operator interpretations of topological
vertices
  • A-model Lattice chiral algebra / Heisenberg
    algebra
  • Okounkov-Reshetikhin-Vafa (hep-th/0309208)
  • Eguchi-Kanno (hep-th/0312234)
  • B-model W-algebra
  • Aganagic-Dijkgraaf-Klemm-Mariño-Vafa
    (hep-th/0312085)

6
Construction of the moduli space via Heisenberg
algebra I
7
Chepter 2First definition of Beilinson-Drinfeld
chiral algebra
8
Construction of the moduli space via Heisenberg
algebra II
  • E.g. GU(1)n, dual Coxeter number h(G)0, central
    charge1 is constructed
  • In this A-model case, non-commutative lattice
    chiral algebras (local Picard ind-scheme) and
    boson-fermion correspondence, Sugawara-constructi
    on is required
  • Geometric data is the ?-data(?,?,c), ?GG?Z
    bilinear form of lattice,?superline bundle

9
The moduli space via W algebra?
  • Quantum Drinfeld-Sokolov (BRST) reduction is
    known
  • Still under calculation

10
Chapter 3Ran space versus moduli of stable sheaf
/ vector bundles
  • Ziv Ran space R(X)
  • Horizontal section is the vertex operator
  • It consists of finite subset of smooth algebraic
    curve X
  • Factorization of finite number of stalks(n
    punctures) over the moduli space R(X)
  • It is known that Deligne-Mumford compactification
    is necessary for the construction of the moduli
    space of algebraic curve with genus g and n
    punctures

11
Equivalence between factorization algebras and
chiral algebras
12
Conclusion and future direction
  • We do not realize the global structure of the
    moduli spaceChiral homology?
  • Direct relation between the reconstructed moduli
    space of Drinfelds vector bundle and its
    relation to Gelfand-Fuks bundle (Chern-Simons
    theory)
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