English

Matrix Models and Geometry of Moduli Spaces

High Energy Physics - Theory 2008-02-03 v1 alg-geom Algebraic Geometry

Abstract

We give the description of discretized moduli spaces (d.m.s.) \Mcdisc\Mcdisc introduced in \cite{Ch1} in terms of discrete de Rham cohomologies for moduli spaces \Mgn\Mgn. The generating function for intersection indices (cohomological classes) of d.m.s. is found. Classes of highest degree coincide with the ones for the continuum moduli space \Mc\Mc. To show it we use a matrix model technique. The Kontsevich matrix model is the generating function in the continuum case, and the matrix model with the potential Nα\tr(\fr14\LX\LX\fr12log(1X)\fr12X)N\alpha \tr {\bigl(- \fr 14 \L X\L X -\fr12\log (1-X)-\fr12X\bigr)} is the one for d.m.s. In the latest case the effects of Deligne--Mumford reductions become relevant, and we use the stratification procedure in order to express integrals over open spaces \Mdisc\Mdisc in terms of intersection indices, which are to be calculated on compactified spaces \Mcdisc\Mcdisc. We find and solve constraint equations on partition function Z\cal Z of our matrix model expressed in times for d.m.s.: tm±=\tr\fr\dm\d\lm\fr1\e\l1t^\pm_m=\tr \fr{\d^m}{\d\l^m}\fr1{\e^\l-1}. It appears that Z\cal Z depends only on even times and Z[t±]=C(a˚N)\eA\eF({t2n})+F({t2n+}){\cal Z}[t^\pm_\cdot]=C(\aa N) \e^{\cal A}\e^{F(\{t^{-}_{2n}\}) +F(\{-t^{+}_{2n}\})}, where F({t2n±})F(\{t^\pm_{2n}\}) is a logarithm of the partition function of the Kontsevich model, A\cal A being a quadratic differential operator in \ddt2n±\dd{t^\pm_{2n}}.

Keywords

Cite

@article{arxiv.hep-th/9509001,
  title  = {Matrix Models and Geometry of Moduli Spaces},
  author = {L. Chekhov},
  journal= {arXiv preprint arXiv:hep-th/9509001},
  year   = {2008}
}

Comments

40pp., LaTeX, no macros needed, 8 figures in text

R2 v1 2026-07-22T15:56:09.132Z