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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.

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Background

One way to avoid explicit energy-momentum sourcing is to define the gravitational action recursively by expanding the Einstein–Hilbert action around a background metric γ and relating successive terms via functional derivatives. In the flat-background case γ = η, such derivatives are sometimes informally treated as energy-momentum contributions.

The authors point out that it is not established whether these derivatives admit a special-relativistic interpretation as energy-momentum tensors in the Noether sense, which would be needed to justify their physical role as self-energy sources for 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.

GR as a classical spin-2 theory? (2403.08637 - Linnemann et al., 13 Mar 2024) in Section 3.2 (The second horn)