This addendum to the Geometric Relay Programme (GRP) addresses the CMB sector of the programme by showing why the Cosmic Microwave Background can remain effectively identical to the standard GR/ΛCDM description at recombination, while still allowing a geometric reinterpretation of dark matter at lower redshift and galactic scales. The central result is an exact ER → GR decoupling theorem at recombination. In Entangled Relativity, based on the action S = -|C| ∫ Lₘ²/R sqrt (-g) d⁴x, the matter Lagrangian Lₘ is physically active and cannot be replaced by a fluid shortcut without care. The addendum resolves the Lₘ ambiguity for radiation by distinguishing the microscopic electromagnetic Lagrangian from the Hamiltonian energy density. For thermal photons, the electromagnetic Lagrangian satisfies = 0 because of the E ↔ B symmetry of free radiation, while the energy density remains nonzero. Therefore, at z ≈ 1100, baryons and electrons contribute Lₘ ≈ T ≈ -rhob, while thermal photons contribute Lₘ = 0 and Tgamma = 0. This yields Lₘ = T and activates the Minazzoli decoupling condition: Entangled Relativity reduces exactly to General Relativity at recombination. This result is not treated as a weakness of the GRP but as a structural advantage. It explains why the CMB can measure Ωₘ in the standard way, without relay contamination. The Planck value of Ωₘ then feeds the GRP closure chain: Ωₘ → m₀ = sqrt (Ωₘ) H₀ → a₀ = m₀ c / 3 → MOND fixed point. The addendum further proposes that the quantity usually interpreted as cold dark matter, Ωₘ - Ωb ≈ 0. 266, corresponds in the GRP to the relay tension R* (z), scaling as (1+z) ³ in the CRT V3 mixed regime. Thus the same geometric relay field behaves as an effective CDM component at the CMB epoch and as a MOND-like non-linear relay at galactic scales. The work introduces no new free parameter. It does not claim a full replacement of the Boltzmann perturbation calculation. The next required step is a quantitative implementation of the relay perturbations in a modified Boltzmann framework such as hiCLASS or EFTCAMB, with the key failure criterion being whether R* reproduces the observed acoustic peak amplitude ratios, especially Dₗ3/Dₗ2, within observational tolerance. In short: the GRP does not modify the CMB at recombination; it explains why the CMB must look standard, then reinterprets the dark component measured by Planck as a geometric relay tension rather than a particle species.
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Olivier Lane-larquey
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Olivier Lane-larquey (Sat,) studied this question.
synapsesocial.com/papers/6a0aace55ba8ef6d83b705c2 — DOI: https://doi.org/10.5281/zenodo.20232159