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Self-sourcing versus action-level self-coupling in spin-2 self-interaction

Determine whether the interaction of the classical spin-2 field h with an energy-momentum tensor in the self-interaction program should be modeled primarily as self-sourcing at the level of the equations of motion or as self-coupling at the level of the action, noting that for a self-energy-momentum tensor these descriptions are not equivalent.

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Background

Within the self-interaction approach, a free classical spin-2 field h on Minkowski spacetime is iteratively coupled to sources, including its own energy-momentum, with the aim of recovering the Einstein field equations. A crucial step requires specifying how h couples to its energy-momentum tensor, but multiple inequivalent formulations exist.

The authors highlight a conceptual uncertainty: for a self-energy-momentum tensor that contains h itself, describing the interaction as equation-of-motion-level self-sourcing (analogous to electrodynamics) is not equivalent to describing it as action-level self-coupling. Establishing which description is physically primary—and under what principles—remains unresolved within the self-interaction program.

References

Arguably more severely though, and specific to the self-interaction term, it is unclear whether the interaction of h with an energy momentum tensor is to be primarily described as self-sourcing at the level of the equations of motion in analogy to the sourcing notion in electrodynamics, or as self-coupling at the level of action (schematically: $h \cdot T$) in reference to modern particle physics parlance (unlike for a conventional energy-momentum tensor which does not contain $h$ itself, self-interaction and self-coupling are not equivalent in the context of a self-energy-momentum tensor for $h$).

GR as a classical spin-2 theory? (2403.08637 - Linnemann et al., 13 Mar 2024) in Section 2.1 (Ambiguities in derivation)