Matrx Models: a Way to Quantum Moduli Spaces

dc.creatorChekhov, L.
dc.date1993-05-06
dc.date.accessioned2026-07-07T04:19:24Z
dc.date.available2026-07-07T04:19:24Z
dc.descriptionWe give the description of discretized moduli spaces (d.m.s.) $\Mcdisc$ introduced in \cite{Ch1} in terms of a discrete de Rham cohomologies for each moduli space $\Mgn$ of a genus $g$, $n$ being the number of punctures. We demonstrate that intersection indices (cohomological classes) calculated for d.m.s. coincide with the ones for the continuum moduli space $\Mc$ compactified by Deligne and Mumford procedure. To show it we use a matrix model technique. The Kontsevich matrix model is a generating function for these indices in the continuum case, and the matrix model with the potential $Nα\tr {\bigl(- \fr 12 ŁXŁX +\log (1-X)+X\bigr)}$ is the one for d.m.s. In the last case the effects of reductions become relevant, but we use the stratification procedure in order to express integrals over open spaces $\Mdisc$ in terms of intersection indices which are to be calculated on compactified spaces. The coincidence of the cohomological classes for both continuum and d.m.s. models enables us to propose the existence of a quantum group structure on d.m.s. Then d.m.s. are nothing but cyclic (exceptional) representations of a quantum group related to a moduli space $\Mc$. Considering the explicit expressions for integrals of Chern classes over $\Mc$ and $\Mcdisc$ we conjecture that each moduli space $\Mc$ in the Kontsevich parametrization can be presented as a coset $\Mc ={\bf T}^d/G$, $d=3g-3+n$, where ${\bf T}^d$ is some $d$--dimensional complex torus and $G$ is a finite order symmetry group of ${\bf T}^d$.
dc.descriptionLaTeX, 33 pages, preprint PAR-LPTHE 22-93
dc.identifierhttps://arxiv.org/abs/hep-th/9305019
dc.identifierhttp://arxiv.org/abs/hep-th/9305019
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/53537
dc.subjectHigh Energy Physics - Theory
dc.titleMatrx Models: a Way to Quantum Moduli Spaces
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