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D-branes, Exceptional Sheaves and Quivers on Calabi-Yau manifolds: From Mukai to McKay

Suresh Govindarajan, T. Jayaraman

TL;DR

The authors develop a mutation-based framework to generate exceptional coherent sheaves on Calabi–Yau manifolds from a foundational helix built from large-volume monodromy acting on ${ m O}$, thereby reproducing the Gepner-point $ abla$-orbit with $ extstyle abla=igl( extstyle\sum_a l_a=0igr)$. They conjecture that all exceptional bundles arise by successive mutations of this helix and that restricting the mutated objects to the CY hypersurface yields the Gepner-state bundles; in parallel, they show how Beilinson-type quivers emerge in the large-volume regime and how the p-field in the GLSM recovers the McKay quiver at orbifold points. The approach is tested in multiple one- and two-parameter models, including ambient spaces with singularities not inherited by the CY, and the resulting RR-charge data match Gepner-model predictions. The work provides a canonical, phase-aware route to cataloging D-branes across GLSM phases via helices, mutations, and quiver gauge theories, linking geometric and LG/orbifold descriptions. Overall, the method offers a unifying picture of D-brane spectra through Beilinson/Mukai-type quivers and their McKay enhancements, with potential extensions to broader ambient geometries and bound-state structures.

Abstract

We present a method based on mutations of helices which leads to the construction (in the large volume limit) of exceptional coherent sheaves associated with the $(\sum_al_a=0)$ orbits in Gepner models. This is explicitly verified for a few examples including some cases where the ambient weighted projective space has singularities not inherited by the Calabi-Yau hypersurface. The method is based on two conjectures which lead to the analog,in the general case, of the Beilinson quiver for $\BP^n$. We discuss how one recovers the McKay quiver using the gauged linear sigma model (GLSM) near the orbifold or Gepner point in Kähler moduli space.

D-branes, Exceptional Sheaves and Quivers on Calabi-Yau manifolds: From Mukai to McKay

TL;DR

The authors develop a mutation-based framework to generate exceptional coherent sheaves on Calabi–Yau manifolds from a foundational helix built from large-volume monodromy acting on , thereby reproducing the Gepner-point -orbit with . They conjecture that all exceptional bundles arise by successive mutations of this helix and that restricting the mutated objects to the CY hypersurface yields the Gepner-state bundles; in parallel, they show how Beilinson-type quivers emerge in the large-volume regime and how the p-field in the GLSM recovers the McKay quiver at orbifold points. The approach is tested in multiple one- and two-parameter models, including ambient spaces with singularities not inherited by the CY, and the resulting RR-charge data match Gepner-model predictions. The work provides a canonical, phase-aware route to cataloging D-branes across GLSM phases via helices, mutations, and quiver gauge theories, linking geometric and LG/orbifold descriptions. Overall, the method offers a unifying picture of D-brane spectra through Beilinson/Mukai-type quivers and their McKay enhancements, with potential extensions to broader ambient geometries and bound-state structures.

Abstract

We present a method based on mutations of helices which leads to the construction (in the large volume limit) of exceptional coherent sheaves associated with the orbits in Gepner models. This is explicitly verified for a few examples including some cases where the ambient weighted projective space has singularities not inherited by the Calabi-Yau hypersurface. The method is based on two conjectures which lead to the analog,in the general case, of the Beilinson quiver for . We discuss how one recovers the McKay quiver using the gauged linear sigma model (GLSM) near the orbifold or Gepner point in Kähler moduli space.

Paper Structure

This paper contains 26 sections, 89 equations, 3 figures.

Figures (3)

  • Figure 1: Beilinson quiver for $\mathbb P^2$
  • Figure 3: McKay quiver for $\mathbb P^2$
  • Figure 5: Quivers for the flop transition