Abstract

We count the number of bound states of BPS black holes on local Calabi–Yau three-folds involving a Riemann surface of genus g. We show that the corresponding gauge theory on the brane reduces to a q-deformed Yang–Mills theory on the Riemann surface. Following the recent connection between the black hole entropy and the topological string partition function, we find that for a large black hole charge N, up to corrections of O ( e − N ) , Z BH is given as a sum of a square of chiral blocks, each of which corresponds to a specific D-brane amplitude. The leading chiral block, the vacuum block, corresponds to the closed topological string amplitudes. The subleading chiral blocks involve topological string amplitudes with D-brane insertions at ( 2 g − 2 ) points on the Riemann surface analogous to the Ω points in the large N 2d Yang–Mills theory. The finite N amplitude provides a non-perturbative definition of topological strings in these backgrounds. This also leads to a novel non-perturbative formulation of c = 1 non-critical string at the self-dual radius.

Highlights

  • Counting of 4-dimensional BPS black hole microstates arising upon compactifications of type II superstrings on Calabi-Yau 3-folds has been recently connected to topological string amplitudes in a highly non-trivial way [1]

  • In particular it has been argued that for a large black hole charge N and to all order in 1/N expansion, the mixed ensemble partition function ZBH of BPS black holes is related to topological string amplitudes Ztop: ZBH = |Ztop|2

  • Once again we find that the topological gauge theory on the brane reduces to 2d Yang-Mills theory on the Riemann surface, with one additional subtlety: the Yang-Mills theory is q-deformed ! We ask if the relation (1.1) holds in this case

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Summary

Introduction

Counting of 4-dimensional BPS black hole microstates arising upon compactifications of type II superstrings on Calabi-Yau 3-folds has been recently connected to topological string amplitudes in a highly non-trivial way [1]. Note that dq(R)qk(R)/4 is the same as the topological vertex amplitude CR,0,0 [5] with all but one representation set to be trivial: dq(R)qk(R)/4 = CR,0,0 = WR0 This is a consistency check, since in this case we are considering the A-model corresponding to stack of D-branes on Calabi-Yau X = C3. Because the pant and the annulus are all diagonal in representations, the complex structure moduli of the Riemann surface one builds by cutting and pasting do not enter in the resulting topological string amplitudes This is as it should be, since these correspond to the complex structure moduli of Calabi-Yau, and perturbative A-model topological string amplitudes better not depend on them.

D-branes in the Fiber
An Alternative Derivation
The q-Deformed 2d YM Theory I
The q-Deformed 2d YM Theory II
Black Hole Entropy
Large N Limit of ZqYM and the Relation to Perturbative Topological Strings
Large N Expansion and Perturbative Topological String
Topological String Interpretation
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