Abstract

We make a proposal for calculating refined Gopakumar-Vafa numbers (GVN) on elliptically fibered Calabi-Yau 3-folds based on refined holomorphic anomaly equations. The key examples are smooth elliptic fibrations over (almost) Fano surfaces. We include a detailed review of existing mathematical methods towards defining and calculating the (unrefined) Gopakumar-Vafa invariants (GVI) and the GVNs on compact Calabi-Yau 3-folds using moduli of stable sheaves, in a language that should be accessible to physicists. In particular, we discuss the dependence of the GVNs on the complex structure moduli and on the choice of an orientation. We calculate the GVNs in many instances and compare the B-model predictions with the geometric calculations. We also derive the modular anomaly equations from the holomorphic anomaly equations by analyzing the quasi-modular properties of the propagators. We speculate about the physical relevance of the mathematical choices that can be made for the orientation.

Highlights

  • We make a proposal for calculating refined Gopakumar-Vafa numbers (GVN) on elliptically fibered Calabi-Yau 3-folds based on refined holomorphic anomaly equations

  • We include a detailed review of existing mathematical methods towards defining and calculating the Gopakumar-Vafa invariants (GVI) and the GVNs on compact Calabi-Yau 3folds using moduli of stable sheaves, in a language that should be accessible to physicists

  • The B-model approach using a refinement [32,33,34] of BCOV (Bershadsky-CecottiOoguri-Vafa) holomorphic anomaly equations [35] supplemented by boundary conditions at the points of parabolic monodromy combined with the modular ansatz can be extended to calculate the refined Gopakumar-Vafa invariants (GVI’s) using the refined holomorphic anomaly equations and refined boundary conditions [32, 34] very efficiently

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Summary

Introduction

The B-model approach using a refinement [32,33,34] of BCOV (Bershadsky-CecottiOoguri-Vafa) holomorphic anomaly equations [35] supplemented by boundary conditions at the points of parabolic monodromy combined with the modular ansatz can be extended to calculate the refined GVI’s using the refined holomorphic anomaly equations and refined boundary conditions [32, 34] very efficiently It applies to local (toric) Calabi-Yau geometries [32, 34], which have B-model mirror whose compact part is a Riemann surface with a meromorphic differential; see [22, 36].

The physics of Gopakumar-Vafa invariants and their refinements
The geometry of Gopakumar-Vafa invariants and their refinements
Geometric moduli spaces
Instructive examples
Stable sheaves
Genus 0 Gopakumar-Vafa invariants
D-critical loci
Perverse sheaves and D-modules
Orientations
Higher genus Gopakumar-Vafa invariants
Refined Gopakumar-Vafa numbers
Basic properties of elliptic fibred Calabi-Yau 3-fold
Classical topological properties
The refined theory on elliptic fibration over P2
The genus one amplitude
Higher genus amplitudes
Derivation of modular anomaly equation
More on elliptic fibrations over Fano basis
E42 E6 2Z3
Elliptic fibrations over F0 and F2
Derivation of modular anomaly equation: general case
Base degree 0
Base curves of genus 0
Conclusion
The refined GV numbers for some low degrees
The refined GV numbers for some low genera
B Refined GV numbers for elliptic fibration over F1

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