Large gauge transformations, gauge invariance, and the QCD θ_(YM)-term

The eliminative view of gauge degrees of freedom -- the view that they arise solely from descriptive redundancy and are therefore eliminable from the theory -- is a lively topic of debate in the philosophy of physics. Recent work attempts to leverage properties of the QCD $\theta_{\text{YM}}$-term to provide a novel argument against the eliminative view. The argument is based on the claim that the QCD $\theta_{\text{YM}}$-term changes under "large" gauge transformations. Here we review geometrical propositions about fiber bundles that unequivocally falsify these claims: the $\theta_{\text{ YM}}$-term encodes topological features of the fiber bundle used to represent gauge degrees of freedom, but it is fully gauge-invariant. Nonetheless, within the essentially classical viewpoint pursued here, the physical role of the $\theta_{\text{YM}}$-term shows the physical importance of bundle topology (or superpositions thereof) and thus weighs against (a naive) eliminativism.