Equivariant Cohomotopy implies orientifold tadpole cancellation

TL;DR

This paper develops a mathematical framework using equivariant cohomotopy to rigorously derive and explain M-theory and string theory tadpole cancellation conditions, linking charge quantization to anomaly cancellation.

Contribution

It introduces an equivariant cohomotopy approach to prove brane charge quantization implies tadpole cancellation in M-theory and string theory.

Findings

Charge quantization in equivariant Cohomotopy implies anomaly cancellation.

Unstable equivariant Cohomotopy distinguishes D-brane charges from O-plane charges.

Framework connects mathematical charge quantization with physical tadpole cancellation conditions.

Abstract

There are fundamental open problems in the precise global nature of RR-field tadpole cancellation conditions in string theory. Moreover, the non-perturbative lift as M5/MO5-anomaly cancellation in M-theory had been based on indirect plausibility arguments,lacking a microscopic underpinning in M-brane charge quantization. We provide a framework for answering these questions, crucial not only for mathematical consistency but also for phenomenological accuracy of string theory, by formulating the M-theory C-field on flat M-orientifolds in the generalized cohomology theory called Equivariant Cohomotopy. This builds on our previous results for smooth but curved spacetimes, showing in that setting that charge quantization in twisted Cohomotopy rigorously implies a list of expected anomaly cancellation conditions. Here we further expand this list by proving that brane charge quantization in unstable equivariant Cohomotopy implies the anomaly cancellation conditions for M-branes and D-branes on flat orbi-orientifolds. For this we (a) use an unstable refinement of the equivariant Hopf-tom Dieck theorem to derive local/twisted tadpole cancellation, and (b) the lift to super-differential cohomology to establish global/untwisted tadpole cancellation. Throughout, we use (c) the unstable Pontrjagin-Thom theorem to identify the brane/O-plane configurations encoded in equivariant Cohomotopy and (d) the Boardman homomorphism to equivariant K-theory to identify Chan-Paton representations of D-brane charge. We find that unstable equivariant Cohomotopy, but not its image in K-theory, distinguishes D-brane charge from the finite set of types of O-plane charges.