Special-relativistic status of the recursive functional derivative as an energy-momentum tensor
Determine whether the functional derivative δS_{n−1}[γ,h]/δg^{μν} evaluated at γ = η, arising in the recursive expansion of the Einstein–Hilbert action, can be interpreted within special relativity as an energy-momentum tensor derived via Noether’s theorem with Poincaré symmetries, thereby justifying its role as a physically meaningful self-energy contribution for the spin-2 field h.
References
As worked out before, it is not clear then that \frac{\delta S_{n-1} [\gamma, h]}{\delta g{\mu \nu}\vert_{\gamma = \eta}$ can be associated with any sort of special relativistic concept of energy-momentum tensors (as usually done via Noether's theorem for the special relativistic context, i.e., in relation to the Poincaré symmetries)---and thus regarded as clearly physically sensible contributions to $h$'s self-energy.