Gauge potentials on the M5 brane in twisted equivariant cohomotopy

TL;DR

This paper explores the global structure of gauge potentials and transformations on M5 branes in M-theory using twisted equivariant cohomotopy, extending previous models to include background gravity and orbifolds.

Contribution

It generalizes the cohomotopy-based flux quantization framework to include twisting by gravity and orbifolds, explicitly constructing gauge potentials and transformations.

Findings

Reproduces traditional gauge potential formulas via homotopy theory

Extends flux quantization to twisted and equivariant cohomotopy

Ensures consistency with Bianchi identities

Abstract

In this article, we work out some variations on the discussion of the C-field flux densities in the Sati-Schreiber program. We start by explaining the need for global completion of the field content: the fluxes, the gauge potentials and the gauge transformations on the worldvolume of a single M5 brane in eleven-dimensional supergravity, and how this is encoded by the choice of flux quantization law. Assuming Hypothesis H that the 4-flux in M-Theory is flux quantized in a non-abelian cohomology theory called 4-cohomotopy, and the three-flux on the M5 brane worldvolume in (twisted) 3-cohomotopy, we generalize some previous calculations known in the literature to include twisting by background gravity and placing M5 branes on orbifolds. We show that the null concordances of cohomotopically charged fluxes give rise to the traditional gauge potentials and the null concordances of concordances give rise to the corresponding gauge transformations via surjections, in the cases of tangentially twisted cohomotopy, twistorial cohomotopy and equivariant twistorial cohomotopy. We construct the surjections explicitly for these cases and check the consistency relations with the corresponding Bianchi identities. Thus, we show how the traditional formulas for the local gauge potentials on M5 brane worldvolume on curved spacetimes and orbifolds are indeed reproduced by the homotopy theory and, as such, become amenable to global completion in cohomotopical charge quantization.