Background independence in gauge theories
Mojtaba Taslimi Tehrani, Jochen Zahn

TL;DR
This paper explores how background independence can be maintained in gauge theories at the quantum level, analyzing obstructions in Yang-Mills and gravity, and proposing a geometrical framework for defining background-independent observables.
Contribution
It introduces a geometrical formulation of background independence using flat connections on the observable algebra bundle, and analyzes quantum obstructions in Yang-Mills and gravity.
Findings
All potential obstructions in Yang-Mills can be removed by renormalization.
Gravity exhibits infinitely many potential obstructions due to non-renormalizability.
The framework clarifies the conditions for background independence at the quantum level.
Abstract
Classical field theory is insensitive to the split of the field into a background configuration and a dynamical perturbation. In gauge theories, the situation is complicated by the fact that a covariant (w.r.t. the background field) gauge fixing breaks this split independence of the action. Nevertheless, background independence is preserved on the observables, as defined via the BRST formalism, since the violation term is BRST exact. In quantized gauge theories, however, BRST exactness of the violation term is not sufficient to guarantee background independence, due to potential anomalies. We define background independent observables in a geometrical formulation as flat sections of the observable algebra bundle over the manifold of background configurations, with respect to a flat connection which implements background variations. A theory is then called background independent if such a…
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