The M-Theory Three-Form and Singular Geometries

TL;DR

This paper proposes an alternative framework for understanding singularities in M-theory compactifications, linking the three-form to bundle Chern-Simons forms and revealing new degrees of freedom without M2-branes.

Contribution

It introduces a novel model connecting the M-theory three-form to bundle Chern-Simons forms, explaining phenomena like gauge symmetry enhancement and charged matter without wrapped M2-branes.

Findings

Reveals new degrees of freedom at singularities

Explains gauge symmetry enhancement via bundle restrictions

Provides a gauge-fixing approach using instanton equations

Abstract

While M- and F-theory compactifications describe a much larger class of vacua than perturbative string compactifications, they typically need singularities to generate non-abelian gauge fields and charged matter. The physical explanation involves M2-branes wrapped on vanishing cycles. Here we seek an alternative explanation that could address outstanding issues such as the description of nilpotent branches, stability walls, frozen singularities and so forth. To this end we use a model in which the three-form is related to the Chern-Simons form of a bundle. The model has a one-form non-abelian gauge symmetry which normally eliminates all the degrees of freedom associated to the bundle. However by restricting the transformations to preserve the bundle along the vanishing cycles, we may get new degrees of freedom associated to singularities, without appealing to wrapped M2-branes. The analysis can be simplified by gauge-fixing the one-form symmetry using higher-dimensional instanton equations. We explain how this mechanism leads to the natural emergence of phenomena such as enhanced ADE gauge symmetries, nilpotent branches, charged matter fields and their holomorphic couplings.