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Shadow Theory

Bulk-to-Brane Projection, Dynamical Nonclosure, and Observable Residues in Randall–Sundrum Gravity

Conclusion

Jeremy RodgersSection 17 of 18Original PDF ↗Publication DOI ↗

Conclusion

Minimal positive-tension RS2 contains a complete source-projection antecedent. In that model, the projection from gauge-reduced bulk gravity to the instantaneous brane state removes genuine gravitational degrees of freedom: a remote transverse-traceless bulk wave, whose existence is established by an explicit KK spectral construction, supplies a same-readout, different-future pair, so no deterministic evolution law exists on that instantaneous state over the full source domain. Gauss–Codazzi projection and Israel matching derive, rather than posit, CμνRS=κ54Πμν−Eμν.\mathcal C^{\mathrm{RS}}_{\mu\nu}=\kappa_5^4\Pi_{\mu\nu}-E_{\mu\nu}. Its local nonlinear part gives the exact positive ρ2\rho^2 correction; its bulk Weyl part carries the completion data and the retarded KK memory. The same source scale ℓ\ell fixes the leading weak-field potentials, producing the parameter-eliminated relation AΨ=AΦ/2,B=κ44AΦ/24,A_\Psi=A_\Phi/2, \qquad B=\kappa_4^4A_\Phi/24 , a genuine, falsifiable residue linking two otherwise independent observational regimes. This is the strongest quantitative result obtained here.

The strongest possible interpretation is nevertheless bounded by Lemma 11.1: every source model induces, by pushforward, a brane-only path law with identical brane statistics, and RS2 makes that obstruction concrete through its four-dimensional CFT description, which reproduces the same 1/r31/r^3 residue. The result is therefore positive at the level of model-relative source projection and nonclosure, and negative at the level of unrestricted ontological discrimination. Absent an independently motivated restriction on the admissible brane-only theory class, no brane observation can establish that the source representation is ontologically fundamental; and establishing that nature realizes this antecedent at all requires empirical selection of RS2, or of another source model with comparably specific residues. The conditions under which the positive results hold are stated once, in Section 15.

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