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The Crispy Fried Chicken Status Board

One claim: a₀ = κ c √(G ρΛ), with κ = ½ fitted, not derived. A cold component of mass (Ωch² ≈ 0.12) is still required, and no dark-matter particle is added. Every tile restates a verdict from a committed script whose pass/fail rules were frozen before the data were read. Updated 5 October 2026.

Status board: every test of the theory as a coloured tile
Pass
Gravity waves at light speed, binary pulsars, solar-system tests, matter conservation, rotation curves (SPARC), local a₀ from MeerKAT (0.9–1.3 × 10⁻¹⁰ m/s²), weak lensing, clusters, Andromeda and Local Volume dwarfs, and candidate B’s large-scale structure growth (it matches ΛCDM and Planck CMB lensing).
Conditional
Well-posedness, strong coupling, structural order, radiative stability (needs new physics below ~10⁹ GeV), and black holes: EHT and LIGO are matched, but a moving black hole keeps a hidden, Planck-scale defect on its innermost horizon.
Not decidable yet
Whether a₀ changes over cosmic time: at high redshift the gas-mass uncertainty is larger than the gap between the flat line and the rival. Also the massive ellipticals, whose gap is not significant with measured tracers.
Fails
Milky Way ultra-faint dwarfs: about 2× too fast, 3.8σ, confirmed from the raw data; tides, binary stars, stellar masses and the Milky Way’s pull are all ruled out. Also structure growth for the bare relativistic theory without the bound-only switch.
Open
Gaia DR4 wide binaries (2 Dec 2026, pre-registered), why κ = ½, what sets the cold-mass amount, and ownership from an action.

Does a₀ change over cosmic time?

The theory predicts a flat line; the rival grows with the expansion rate H(z). The two separate at redshift 2–5, where today’s gas measurements are not yet precise enough to tell them apart.

a₀ against redshift: flat line versus the a₀ ∝ H(z) rival

Full guide and sources: the explainer on GitHub. Next decisive test: Gaia DR4, 2 December 2026.