Secondary cohomology operations and the loop space cohomology
Samson Saneblidze
TL;DR
The paper introduces secondary cohomology operations on $H^*(X; \mathbb{Z}_p)$ and shows how they form a Hopf algebra that controls loop space cohomology via $H^*(\Omega X; \mathbb{Z}_p)$. A mod $p$ filtered Hirsch model built from a minimal Hirsch resolution $RH$ and a perturbation $h$ yields a dg Hopf algebra model, whose bar-construction recovers the loop space cohomology and its coproduct. The secondary operations $\psi_{r,n}$ and the generators $\omega_{r,n}(x)$ are defined through the filtered Hirsch framework, enabling explicit power relations and kernel descriptions tied to Bockstein data. The authors apply the theory to compute the mod $p$ loop cohomology of the exceptional group $F_4$ at $p=2$ and $p=3$, illustrating a practical, constructive method for determining loop space cohomology and its Hopf-algebra structure in challenging cases.
Abstract
Motivated by the loop space cohomology we construct the secondary operations on the cohomology $H^*(X; \mathbb{Z}_p)$ to be a Hopf algebra for a simply connected space $X.$ The loop space cohomology ring $H^*(ΩX; \mathbb{Z}_p)$ is calculated in terms of generators and relations. This answers to A. Borel's decomposition of a Hopf algebra into a tensor product of the monogenic ones in which the heights of generators are determined by means of the action of the primary and secondary cohomology operations on $H^*(X;\mathbb{Z}_p).$ An application for calculating of the loop space cohomology of the exceptional group $F_4$ is given.
